(Generated on Mon Jan 28 2019 16:58:31 for HEPfit by
1.8.14)
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(Generated on Mon Jan 28 2019 16:58:31 for HEPfit by
1.8.14)
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A model class for new physics in the form of the dimension-six effective Lagrangian. More...
#include <NPSMEFTd6.h>
A model class for new physics in the form of the dimension-six effective Lagrangian.
This is a Model class containing parameters and functions associated with the general dimension-six effective Lagrangian. (Use the model name "NPSMEFTd6_LFU_QFU" to asumme lepton and quark flavour universality)
In this class we consider the dimension-six effective Lagrangian
\[ \mathcal{L}_\mathrm{eff} = \mathcal{L}_\mathrm{SM} + \sum_i \frac{C_i}{\Lambda^2} \mathcal{O}_i. \]
The implementation is written in the basis of [88]. For convenience, the parameterization also includes operators appearing in other common bases. In particular, the complete set of parameters containts 2 redundancies, given by coefficients \(C_{DHB} \) and \(C_{DHW} \), which correspond to operators not included in the basis of [88]. For meaningful physical results one must make sure to include only a complete set of interactions in a given analysis.
After creating an instance of the current class with the constructor NPSMEFTd6(), it is required to call the initialization method InitializeModel(). In the Monte Carlo run, the constructor as well as the initialization method are called in InputParser::ReadParameters().
The model parameters of NPSMEFTd6 are summarized below:
| Label | LaTeX symbol | Description |
|---|---|---|
| CG | \(C_{G} \) | The coefficient of the operator \({\cal O}_{G}=f_{ABC}G_{\mu}^{A\nu} G_{\nu}^{B\rho}W_{\rho}^{C\mu}\). |
| CW | \(C_{W} \) | The coefficient of the operator \({\cal O}_{W}=\varepsilon_{abc}W_{\mu}^{a\nu} W_{\nu}^{b\rho}W_{\rho}^{b\mu}\). |
| C2B | \(C_{2B} \) | The coefficient of the operator \({\cal O}_{2B}=\frac 12 (\partial_\rho B_{\mu\nu})^2\). |
| C2W | \(C_{2W} \) | The coefficient of the operator \({\cal O}_{2W}=\frac 12 (D_\rho W_{\mu\nu}^{a})^2\). |
| CHG | \(C_{HG} \) | The coefficient of the operator \({\cal O}_{HG}=\big(H^\dagger H\big)G_{\mu\nu}^A G^{A\mu\nu}\). |
| CHW | \(C_{HW} \) | The coefficient of the operator \({\cal O}_{HW}=\big(H^\dagger H\big)W_{\mu\nu}^a W^{a\mu\nu}\). |
| CHB | \(C_{HB} \) | The coefficient of the operator \({\cal O}_{HB}=\big(H^\dagger H\big)B_{\mu\nu} B^{\mu\nu}\). |
| CDHB | \(C_{DHB} \) | The coefficient of the operator \({\cal O}_{DHB}=i\big(D^\mu H^\dagger D^\nu H\big) B_{\mu\nu}\). |
| CDHW | \(C_{DHW}\) | The coefficient of the operator \({\cal O}_{DHW}=i\big(D^\mu H^\dagger \tau^a D^\nu H\big) W_{\mu\nu}^a\). |
| CWB | \(C_{WB} \) | The coefficient of the operator \({\cal O}_{HWB}=\big(H^\dagger\tau^a H\big)W_{\mu\nu}^a B^{\mu\nu}\). |
| CHD | \(C_{HD}\) | The coefficient of the operator \({\cal O}_{HD}=\big|H^\dagger D_\mu H\big|^2\). |
| CHbox | \(C_{H\Box}\) | The coefficient of the operator \({\cal O}_{H\Box}=\big(H^\dagger H\big)\Box\big(H^\dagger H\big)\). |
| CH | \(C_{H}\) | The coefficient of the operator \({\cal O}_{H}=\big(H^\dagger H\big)^3\). |
| CHL1_kk, CHL1_klr, CHL1_kli | \( (C_{HL}^{(1)})_{kk}, \mbox{Re}\big[(C_{HL}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(1)})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HL}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{L^i}\,\gamma^\mu L^j\big)\), for \(i,j=1,2,3\). |
| CHL3_kk, CHL3_klr, CHL3_kli | \( (C_{HL}^{(3)})_{kk}, \mbox{Re}\big[(C_{HL}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HL}^{(3)})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HL}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{L^i}\,\gamma^\mu \tau^a L^j\big)\), for \(i,j=1,2,3\). |
| CHe_kk, CHe_klr, CHe_kli | \( (C_{He})_{kk}, \mbox{Re}\big[(C_{He})_{kl}\big], \mbox{Im}\big[(C_{He})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{He})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{E^i}\,\gamma^\mu E^j\big)\), for \(i,j=1,2,3\). |
| CHQ1_kk, CHQ1_klr, CHQ1_kli | \( (C_{HQ}^{(1)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(1)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(1)})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HQ}^{(1)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{Q^i}\,\gamma^\mu Q^j\big)\), for \(i,j=1,2,3\). |
| CHQ3_kk, CHQ3_klr, CHQ3_kli | \( (C_{HQ}^{(3)})_{kk}, \mbox{Re}\big[(C_{HQ}^{(3)})_{kl}\big], \mbox{Im}\big[(C_{HQ}^{(3)})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{HQ}^{(3)})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{Q^i}\,\gamma^\mu \tau^a Q^j\big)\), for \(i,j=1,2,3\). |
| CHu_kk, CHu_klr, CHu_kli | \( (C_{Hu})_{kk}, \mbox{Re}\big[(C_{Hu})_{kl}\big], \mbox{Im}\big[(C_{Hu})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hu})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{U^i}\,\gamma^\mu U^j\big)\), for \(i,j=1,2,3\). |
| CHd_kk, CHd_klr, CHd_kli | \( (C_{Hd})_{kk}, \mbox{Re}\big[(C_{Hd})_{kl}\big], \mbox{Im}\big[(C_{Hd})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hd})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{D^i}\,\gamma^\mu D^j\big)\), for \(i,j=1,2,3\). |
| CHud_klr, CHud_kli | \(\mbox{Re}\big[(C_{Hud})_{kl}\big], \mbox{Im}\big[(C_{Hud})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hud})_{ij} =i\big(\widetilde{H}^\dagger D_\mu H\big) \big(\overline{U^i}\,\gamma^\mu D^j\big)\), for \(i,j=1,2,3\). |
| CeH_klr, CeH_kli | \(\mbox{Re}\big[(C_{eH})_{kl}\big], \mbox{Im}\big[(C_{eH})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eH})_{ij} =\big(H^\dagger H\big) \big(\overline{L^i}\,H E^j\big)\), for \(i,j=1,2,3\). |
| CuH_klr, CuH_kli | \(\mbox{Re}\big[(C_{uH})_{kl}\big], \mbox{Im}\big[(C_{uH})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uH})_{ij} =\big(H^\dagger H\big) \big(\overline{Q^i}\,\widetilde{H} U^j\big)\), for \(i,j=1,2,3\). |
| CdH_klr, CdH_kli | \(\mbox{Re}\big[(C_{dH})_{kl}\big], \mbox{Im}\big[(C_{dH})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dH})_{ij} =\big(H^\dagger H\big) \big(\overline{Q^i}\,H D^j\big)\), for \(i,j=1,2,3\). |
| CuG_klr, CuG_kli | \(\mbox{Re}\big[(C_{uG})_{kl}\big], \mbox{Im}\big[(C_{uG})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A U^j\big)\widetilde{H} G_{\mu\nu}^A\), for \(i,j=1,2,3\). |
| CuW_klr, CuW_kli | \(\mbox{Re}\big[(C_{uW})_{kl}\big], \mbox{Im}\big[(C_{uW})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \tau_a U^j\big)\widetilde{H} W_{\mu\nu}^a\), for \(i,j=1,2,3\). |
| CuB_klr, CuB_kli | \(\mbox{Re}\big[(C_{uB})_{kl}\big], \mbox{Im}\big[(C_{uB})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} U^j\big)\widetilde{H} B_{\mu\nu}\), for \(i,j=1,2,3\). |
| CLL_1221, CLL_2112 | \((C_{LL})_{1221,2112}\) | The coefficient of the operator \(({\cal O}_{LL})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{L^k}\,\gamma_\mu L^l\big)\), for \(ijkl=1221,2112\). |
| CLQ1 | \(C_{LQ}^{(1)}\) | The coefficient of the operator \(({\cal O}_{LQ}^{(1)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)\). |
| CLQ3 | \(C_{LQ}^{(3)}\) | The coefficient of the operator \(({\cal O}_{LQ}^{(3)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu \tau_a L^j\big) \big(\overline{Q^k}\,\gamma_\mu \tau_a Q^l\big)\). |
| Cee | \(C_{EE}\) | The coefficient of the operator \(({\cal O}_{EE})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| Ceu | \(C_{EU}\) | The coefficient of the operator \(({\cal O}_{EU})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\). |
| Ced | \(C_{ED}\) | The coefficient of the operator \(({\cal O}_{ED})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\). |
| CLe | \(C_{LE}\) | The coefficient of the operator \(({\cal O}_{LE})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| CLu | \(C_{LU}\) | The coefficient of the operator \(({\cal O}_{LU})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\). |
| CLd | \(C_{LD}\) | The coefficient of the operator \(({\cal O}_{LD})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\). |
| CQe | \(C_{QE}\) | The coefficient of the operator \(({\cal O}_{QE})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| Lambda_NP | \(\Lambda \) | The new physics scale. |
| BrHinv | Br \((H\to invisible)\) | The branching ratio of invisible Higgs decays. Only the absolute value of this parameter is considered.(Not part of the EFT. Only for tests.) |
| BrHexo | Br \((H\to exotic)\) | The branching ratio of exotic Higgs decays. Only the absolute value of this parameter is considered. (Not part of the EFT. Only for tests.) |
| dg1Z | \(\delta g_{1Z}\) | Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.) |
| dKappaga | \(\delta \kappa_{\gamma}\) | Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.) |
| lambZ | \(\lambda_{Z}\) | Independent contribution to aTGC. (extra contribution to the one from the EFT. Only for tests.) |
| eXint | \(\varepsilon_{X}^{int}\) | The relative intrinsic theoretical uncertainty for the process X. (Only for Higgs observables and assumed to be constant in the energy.) |
| eXpar | \(\varepsilon_{X}^{par}\) | The relative parametric theoretical uncertainty for the process X. (Only for Higgs observables and assumed to be constant in the energy.) |
| eVBFE_i | \(\varepsilon_{VBF}^i(E)\) | The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the VBF production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i=g_{HZZ}^{(1,2,3)}, g_{HZA}^{(1,2)}, g_{HAA}, g_{HWW}^{(1,2,3)}, g_{Hgg}, g_{HZuu,HZdd}^{L,R}, g_{HWud}^{L}, g_{Zuu,Zdd}^{L,R}, g_{Wud}^{L})\) |
| eWHE_i | \(\varepsilon_{WH}^i(E)\) | The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the WH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i= g_{HWW}^{(1,2,3)}, g_{HWud}^{L}, g_{Wud}^{L})\) |
| eZHE_i | \(\varepsilon_{ZH}^i(E)\) | The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the ZH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i=g_{HZZ}^{(1,2,3)}, g_{HZA}^{(1,2)}, g_{HZuu,HZdd}^{L,R}, g_{Zuu,Zdd}^{L,R})\) |
| ettHE_i | \(\varepsilon_{ttH}^i(E)\) | The theoretical uncertainty in the coefficient multiplying the effective coupling \(g_i\) in the ttH production cross section at Tevatron ( \(E=2\)) or the LHC ( \(E=78\)). \((g_i= g_{Htt}, g_{Hgg})\) |
Where the hermitian derivatives are defined as
\[ H^\dagger i \overset{\leftrightarrow}{D}_\mu H\equiv H^\dagger i(D_\mu - \overset{\leftarrow}{D}_\mu)H \]
and
\[ H^\dagger i \overset{\leftrightarrow}{D^a_\mu} H\equiv H^\dagger i (\tau^a D_\mu - \overset{\leftarrow}{D}_\mu \tau^a)H. \]
Alternatively, when using the model name "NPSMEFTd6_LFU_QFU", where lepton and quark flavour universality are assumed (except for \((C_{fH})_{ij},~f=e,u,d\) which are assumed to be diagonal only), the parameters to be used as inputs for the dimension six coefficients are the following:
| Label | LaTeX symbol | Description |
|---|---|---|
| CG | \(C_{G} \) | The coefficient of the operator \({\cal O}_{G}=f_{ABC}G_{\mu}^{A\nu} G_{\nu}^{B\rho}W_{\rho}^{C\mu}\). |
| CW | \(C_{W} \) | The coefficient of the operator \({\cal O}_{W}=\varepsilon_{abc}W_{\mu}^{a\nu} W_{\nu}^{b\rho}W_{\rho}^{b\mu}\). |
| C2B | \(C_{2B} \) | The coefficient of the operator \({\cal O}_{2B}=\frac 12 (\partial_\rho B_{\mu\nu})^2\). |
| C2W | \(C_{2W} \) | The coefficient of the operator \({\cal O}_{2W}=\frac 12 (D_\rho W_{\mu\nu}^{a})^2\). |
| CHG | \(C_{HG} \) | The coefficient of the operator \({\cal O}_{HG}=\big(H^\dagger H\big)G_{\mu\nu}^A G^{A\mu\nu}\). |
| CHW | \(C_{HW} \) | The coefficient of the operator \({\cal O}_{HW}=\big(H^\dagger H\big)W_{\mu\nu}^a W^{a\mu\nu}\). |
| CHB | \(C_{HB} \) | The coefficient of the operator \({\cal O}_{HB}=\big(H^\dagger H\big)B_{\mu\nu} B^{\mu\nu}\). |
| CDHB | \(C_{DHB} \) | The coefficient of the operator \({\cal O}_{DHB}=i\big(D^\mu H^\dagger D^\nu H\big) B_{\mu\nu}\). |
| CDHW | \(C_{DHW}\) | The coefficient of the operator \({\cal O}_{DHW}=i\big(D^\mu H^\dagger \tau^a D^\nu H\big) W_{\mu\nu}^a\). |
| CWB | \(C_{WB} \) | The coefficient of the operator \({\cal O}_{HWB}=\big(H^\dagger\tau^a H\big)W_{\mu\nu}^a B^{\mu\nu}\). |
| CHD | \(C_{HD}\) | The coefficient of the operator \({\cal O}_{HD}=\big|H^\dagger D_\mu H\big|^2\). |
| CHbox | \(C_{H\Box}\) | The coefficient of the operator \({\cal O}_{H\Box}=\big(H^\dagger H\big)\Box\big(H^\dagger H\big)\). |
| CH | \(C_{H}\) | The coefficient of the operator \({\cal O}_{H}=\big(H^\dagger H\big)^3\). |
| CHL1 | \( (C_{HL}^{(1)})_{ii} \) | The coefficient of the operator \(({\cal O}_{HL}^{(1)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{L^i}\,\gamma^\mu L^i\big)\) (flavor universal). |
| CHL3 | \( (C_{HL}^{(3)})_{ii} \) | The coefficient of the operator \(({\cal O}_{HL}^{(3)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{L^i}\,\gamma^\mu \tau^a L^i\big)\) (flavor universal). |
| CHe | \( (C_{He})_{ii} \) | The coefficient of the operator \(({\cal O}_{He})_{ij} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{E^i}\,\gamma^\mu E^i\big)\) (flavor universal). |
| CHQ1 | \( (C_{HQ}^{(1)})_{ii} \) | The coefficient of the operator \(({\cal O}_{HQ}^{(1)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{Q^i}\,\gamma^\mu Q^i\big)\) (flavor universal). |
| CHQ3 | \( (C_{HQ}^{(3)})_{ii}\) | The coefficient of the operator \(({\cal O}_{HQ}^{(3)})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D^a_\mu} H\big) \big(\overline{Q^i}\,\gamma^\mu \tau^a Q^i\big)\) (flavor universal). |
| CHu | \( (C_{Hu})_{ii} \) | The coefficient of the operator \(({\cal O}_{Hu})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{U^i}\,\gamma^\mu U^i\big)\) (flavor universal). |
| CHd | \( (C_{Hd})_{ii} \) | The coefficient of the operator \(({\cal O}_{Hd})_{ii} =i\big(H^\dagger \overset{\leftrightarrow}{D}_\mu H\big) \big(\overline{D^i}\,\gamma^\mu D^i\big)\) (flavor universal). |
| CHud_r, CHud_i | \(\mbox{Re}\big[(C_{Hud})_{ii}\big], \mbox{Im}\big[(C_{Hud})_{ii}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{Hud})_{ii} =i\big(\widetilde{H}^\dagger D_\mu H\big) \big(\overline{U^i}\,\gamma^\mu D^i\big)\) (flavor universal). |
| CeH_jjr, CeH_jji | \(\mbox{Re}\big[(C_{eH})_{jj}\big], \mbox{Im}\big[(C_{eH})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{eH})_{jj} =\big(H^\dagger H\big) \big(\overline{L^j}\,H E^j\big)\) (flavor universal). |
| CuH_jjr, CuH_jji | \(\mbox{Re}\big[(C_{uH})_{jj}\big], \mbox{Im}\big[(C_{uH})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uH})_{jj} =\big(H^\dagger H\big) \big(\overline{Q^j}\,\widetilde{H} U^j\big)\) (flavor universal). |
| CdH_jjr, CdH_jji | \(\mbox{Re}\big[(C_{dH})_{jj}\big], \mbox{Im}\big[(C_{dH})_{jj}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{dH})_{jj} =\big(H^\dagger H\big) \big(\overline{Q^j}\,H D^j\big)\) (flavor universal). |
| CuG_klr, CuG_kli | \(\mbox{Re}\big[(C_{uG})_{kl}\big], \mbox{Im}\big[(C_{uG})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uG})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} T_A U^j\big)\widetilde{H} G_{\mu\nu}^A\), for \(i,j=1,2,3\). |
| CuW_klr, CuW_kli | \(\mbox{Re}\big[(C_{uW})_{kl}\big], \mbox{Im}\big[(C_{uW})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uW})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} \tau_a U^j\big)\widetilde{H} W_{\mu\nu}^a\), for \(i,j=1,2,3\). |
| CuB_klr, CuB_kli | \(\mbox{Re}\big[(C_{uB})_{kl}\big], \mbox{Im}\big[(C_{uB})_{kl}\big] \) | The real and imaginary parts of the coefficient of the operator \(({\cal O}_{uB})_{ij} =\big(\overline{Q^i}\sigma^{\mu\nu} U^j\big)\widetilde{H} B_{\mu\nu}\), for \(i,j=1,2,3\). |
| CLL | \((C_{LL})_{1221,2112}\) | The coefficient of the operator \(({\cal O}_{LL})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{L^k}\,\gamma_\mu L^l\big)\), for \(ijkl=1221,2112\). |
| CLQ1 | \(C_{LQ}^{(1)}\) | The coefficient of the operator \(({\cal O}_{LQ}^{(1)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{Q^k}\,\gamma_\mu Q^l\big)\). |
| CLQ3 | \(C_{LQ}^{(3)}\) | The coefficient of the operator \(({\cal O}_{LQ}^{(3)})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu \tau_a L^j\big) \big(\overline{Q^k}\,\gamma_\mu \tau_a Q^l\big)\). |
| Cee | \(C_{EE}\) | The coefficient of the operator \(({\cal O}_{EE})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| Ceu | \(C_{EU}\) | The coefficient of the operator \(({\cal O}_{EU})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\). |
| Ced | \(C_{ED}\) | The coefficient of the operator \(({\cal O}_{ED})_{ijkl}=\big(\overline{E^i}\,\gamma^\mu E^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\). |
| CLe | \(C_{LE}\) | The coefficient of the operator \(({\cal O}_{LE})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| CLu | \(C_{LU}\) | The coefficient of the operator \(({\cal O}_{LU})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{U^k}\,\gamma_\mu U^l\big)\). |
| CLd | \(C_{LD}\) | The coefficient of the operator \(({\cal O}_{LD})_{ijkl}=\big(\overline{L^i}\,\gamma^\mu L^j\big) \big(\overline{D^k}\,\gamma_\mu D^l\big)\). |
| CQe | \(C_{QE}\) | The coefficient of the operator \(({\cal O}_{QE})_{ijkl}=\big(\overline{Q^i}\,\gamma^\mu Q^j\big) \big(\overline{E^k}\,\gamma_\mu E^l\big)\). |
| Lambda_NP | \(\Lambda \) | The new physics scale. |
| BrHinv | Br \((H\to invisible)\) | The branching ratio of invisible Higgs decays. (Not part of the EFT. Only for tests.) |
| BrHexo | Br \((H\to exotic)\) | The branching ratio of exotic Higgs decays. (Not part of the EFT. Only for tests.) |
(The parameters associated to the theoretical uncertainties: \(\varepsilon_{X}^{int}\), \(\varepsilon_{X}^{par}\) and \(\varepsilon_{X}^i(E)\), are the same for both "NPSMEFTd6" and "NPSMEFTd6_LFU_QFU".)
The Flags of NPSMEFTd6 are summarized below:
| Label | Value | Description |
|---|---|---|
| QuadraticTerms | TRUE / FALSE | This flag is set to TRUE if the quadratic terms in Higgs cross sections and widths are switched on. The default value is FALSE; new physics contributions are linearized. |
| RotateCHWCHB | TRUE / FALSE | This flag is set to TRUE if using {sW2*CHW+cW2*CHB, -cW2*CHW+sW2*CHB} instead of {CHW, CHB} as floating parameters. The default value is FALSE. |
| PartialQFU | TRUE / FALSE | This flag is set to TRUE if using CHQ1_11=CHQ1_22, CHQ3_11=CHQ3_22, CHU_11=CHU_22, CHD_11=CHD_22, CHud_11=CHud_22.} Only applies in the Non QFU case. In that case only the (1,1) component is taken into account. The default value is FALSE. |
| FlavU3OfX | TRUE / FALSE | This flag is set to TRUE if using \(U(3)^5\) flavour symmetry relations in the coefficients of the operators \(O_{fH}\) and \(O_{fV}\). If TRUE, the operator coefficient is proportional to the corresponding Yukawa matrix (diagonal), with the proportionality coefficient given by the Model parameter corresponding to the coefficient of third family. (Implemented only for the real and diagonal elements of the \(O_{fH}\) and \(O_{fV}\) operators.) The default value is FALSE. |
| FlagUnivOfX | TRUE / FALSE | This flag is set to TRUE if using \(U(3)^5\) flavour symmetry relations in the coefficients of the operators \(O_{fH}\) and \(O_{fV}\) plus they are the same for all fermions. If TRUE, all the operator coefficients are proportional to the corresponding Yukawa matrix (diagonal), with the proportionality coefficient given by the Model parameter corresponding to the coefficients of third family for \(O_{uH}\) and \(O_{uV}\), respectively. (Implemented only for the real and diagonal elements of the \(O_{fH}\) and \(O_{fV}\) operators.) The default value is FALSE. |
| HiggsSM | TRUE / FALSE | This flag is set to TRUE if including dependence on small variations of the SM parameters (dependence is linearized). Available only in selected Higgs observables. The default value is FALSE. |
| LoopHd6 | TRUE / FALSE | This flag is set to TRUE if including modifications in the SM loops in Higgs observables due to the dim 6 interactions. The default value is FALSE. |
| LoopH3d6Quad | TRUE / FALSE | This flag is set to TRUE if including quadratic modifications in the SM loops in Higgs observables due to the dim 6 interactions that contribute to the trilinear Higgs coupling. Works independently of the flag QuadraticTerms (the quadratic contributions are also added if the latter is true). The default value is FALSE. |
See the base classes of the current class.
Definition at line 753 of file NPSMEFTd6.h.
Public Member Functions | |
| gslpp::complex | AH_f (const double tau) const |
| Fermionic loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More... | |
| gslpp::complex | AH_W (const double tau) const |
| W loop function entering in the calculation of the effective \(H\gamma\gamma\) coupling. More... | |
| gslpp::complex | AHZga_f (const double tau, const double lambda) const |
| Fermionic loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| gslpp::complex | AHZga_W (const double tau, const double lambda) const |
| W loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| virtual double | AuxObs_NP1 () const |
| Auxiliary observable AuxObs_NP1 (See code for details.) More... | |
| virtual double | AuxObs_NP2 () const |
| Auxiliary observable AuxObs_NP2 (See code for details.) More... | |
| virtual double | AuxObs_NP3 () const |
| Auxiliary observable AuxObs_NP3 (See code for details.) More... | |
| virtual double | AuxObs_NP4 () const |
| Auxiliary observable AuxObs_NP4 (See code for details.) More... | |
| virtual double | AuxObs_NP5 () const |
| Auxiliary observable AuxObs_NP5 (See code for details.) More... | |
| virtual double | AuxObs_NP6 () const |
| Auxiliary observable AuxObs_NP6 (See code for details.) More... | |
| virtual double | Br_H_exo () const |
| The branching ratio of the of the Higgs into exotic particles. More... | |
| virtual double | Br_H_inv () const |
| The branching ratio of the of the Higgs into invisible particles. More... | |
| virtual double | BrHbbRatio () const |
| The ratio of the Br \((H\to b\bar{b})\) in the current model and in the Standard Model. More... | |
| virtual double | BrHccRatio () const |
| The ratio of the Br \((H\to c\bar{c})\) in the current model and in the Standard Model. More... | |
| virtual double | BrHgagaRatio () const |
| The ratio of the Br \((H\to \gamma\gamma)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHggRatio () const |
| The ratio of the Br \((H\to gg)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHmumuRatio () const |
| The ratio of the Br \((H\to \mu^+\mu^-)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHtautauRatio () const |
| The ratio of the Br \((H\to \tau^+\tau^-)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHtoinvRatio () const |
| The ratio of the Br \((H\to invisible)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHvisRatio () const |
| The ratio of the Br \((H\to visible)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHWffRatio () const |
| The ratio of the Br \((H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| virtual double | BrHWjjRatio () const |
| The ratio of the Br \((H\to W j j)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHWlvRatio () const |
| The ratio of the Br \((H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHWW2l2vRatio () const |
| The ratio of the Br \((H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHWW4fRatio () const |
| The ratio of the Br \((H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| virtual double | BrHWW4jRatio () const |
| The ratio of the Br \((H\to WW^*\to 4j)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHWWRatio () const |
| The ratio of the Br \((H\to WW)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZddRatio () const |
| The ratio of the Br \((H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHZffRatio () const |
| The ratio of the Br \((H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| virtual double | BrHZgaeeRatio () const |
| The ratio of the Br \((H\to Z\gamma\to ee\gamma)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZgallRatio () const |
| The ratio of the Br \((H\to Z\gamma\to ll\gamma)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHZgamumuRatio () const |
| The ratio of the Br \((H\to Z\gamma\to \mu\mu\gamma)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZgaRatio () const |
| The ratio of the Br \((H\to Z\gamma)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZllRatio () const |
| The ratio of the Br \((H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHZuuRatio () const |
| The ratio of the Br \((H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHZvvRatio () const |
| The ratio of the Br \((H\to Z\nu\nu)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZZ2e2muRatio () const |
| The ratio of the Br \((H\to ZZ* \to 2e 2\mu)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZZ4dRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHZZ4eRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4e)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZZ4fRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| virtual double | BrHZZ4lRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHZZ4muRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZZ4uRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More... | |
| virtual double | BrHZZ4vRatio () const |
| The ratio of the Br \((H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. More... | |
| virtual double | BrHZZRatio () const |
| The ratio of the Br \((H\to ZZ)\) in the current model and in the Standard Model. More... | |
| virtual double | cgaga_HB () const |
| The Higgs-basis coupling \(c_{\gamma\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | cgg_HB () const |
| The Higgs-basis coupling \(c_{gg}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual bool | CheckParameters (const std::map< std::string, double > &DPars) |
| A method to check if all the mandatory parameters for NPSMEFTd6 have been provided in model initialization. More... | |
| double | CLL_bottom () const |
| double | CLL_charm () const |
| double | CLL_down () const |
| double | CLL_mu () const |
| double | CLL_strange () const |
| double | CLL_tau () const |
| double | CLL_up () const |
| double | CLR_bottom () const |
| double | CLR_charm () const |
| double | CLR_down () const |
| double | CLR_mu () const |
| double | CLR_strange () const |
| double | CLR_tau () const |
| double | CLR_up () const |
| virtual double | computeGammaTotalRatio () const |
| The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. More... | |
| double | CRL_bottom () const |
| double | CRL_charm () const |
| double | CRL_down () const |
| double | CRL_mu () const |
| double | CRL_strange () const |
| double | CRL_tau () const |
| double | CRL_up () const |
| double | CRR_bottom () const |
| double | CRR_charm () const |
| double | CRR_down () const |
| double | CRR_mu () const |
| double | CRR_strange () const |
| double | CRR_tau () const |
| double | CRR_up () const |
| virtual double | cZBox_HB () const |
| The Higgs-basis coupling \(c_{z\Box}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | cZga_HB () const |
| The Higgs-basis coupling \(c_{z\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | cZZ_HB () const |
| The Higgs-basis coupling \(c_{zz}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | deltaa0 () const |
| The relative correction to the electromagnetic constant at zero momentum, \(\delta \alpha(0)/\alpha(0)\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltaa02 () const |
| The relative correction to the electromagnetic constant at zero momentum, \((\delta \alpha(0)/\alpha(0))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltaaMZ () const |
| The relative correction to the electromagnetic constant at the Z pole, \(\delta \alpha(M_Z^2)/\alpha(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltaaMZ2 () const |
| The relative correction to the electromagnetic constant at the Z pole, \((\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltaaSMZ () const |
| The relative correction to the strong coupling constant at the Z pole, \(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltaaSMZ2 () const |
| The relative correction to the strong coupling constant at the Z pole, \((\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltacZ_HB () const |
| The Higgs-basis coupling \(\delta c_z\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | deltaG1_hWW () const |
| The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\). More... | |
| virtual double | deltaG1_hZA () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\). More... | |
| virtual double | deltaG1_hZARatio () const |
| The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| virtual double | deltaG1_hZZ () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\). More... | |
| virtual double | deltag1ZNP () const |
| The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\). More... | |
| virtual double | deltaG2_hWW () const |
| The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\). More... | |
| virtual double | deltaG2_hZA () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\). More... | |
| virtual double | deltaG2_hZZ () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\). More... | |
| virtual double | deltaG3_hWW () const |
| The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\). More... | |
| virtual double | deltaG3_hZZ () const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\). More... | |
| double | deltag3G () const |
| The new physics contribution to the coupling of the effective interaction \(f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C\). More... | |
| gslpp::complex | deltaG_Aff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| gslpp::complex | deltaG_Gff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| virtual double | deltaG_hAA () const |
| The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\). More... | |
| virtual double | deltaG_hAARatio () const |
| The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| gslpp::complex | deltaG_hAff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| virtual gslpp::complex | deltaG_hff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\). More... | |
| gslpp::complex | deltaG_hGff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| virtual double | deltaG_hgg () const |
| The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\). More... | |
| virtual double | deltaG_hggRatio () const |
| The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value. More... | |
| virtual double | deltaG_hhhRatio () const |
| The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value. More... | |
| gslpp::complex | deltaG_hZff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| gslpp::complex | deltaG_Zff (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\). More... | |
| virtual double | deltaGA_f (const Particle p) const |
| New physics contribution to the neutral-current axial-vector coupling \(g_A^f\). More... | |
| virtual double | deltaGamma_W () const |
| The new physics contribution to the total decay width of the \(W\) boson, \(\delta \Gamma_W\). More... | |
| virtual double | deltaGamma_Wff (const Particle fi, const Particle fj) const |
| The new physics contribution to the decay width of the \(W\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More... | |
| double | deltaGammaHbbRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHbbRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHccRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHccRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHgagaRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHgagaRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHggRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More... | |
| double | deltaGammaHggRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHmumuRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHmumuRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHtautauRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHtautauRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWffRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWffRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWjjRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWjjRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWlvRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWlvRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWW2l2vRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWW2l2vRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWW4fRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWW4fRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWW4jRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWW4jRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWWRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHWWRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZddRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZddRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZeeRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZeeRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZffRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZffRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZgaRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZgaRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZllRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZllRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZmumuRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZmumuRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZuuRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZuuRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZvvRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZvvRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ2e2muRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ2e2muRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4dRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4dRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4eRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4eRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4fRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4fRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4lRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4lRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4muRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4muRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4uRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4uRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4vRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZ4vRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.) More... | |
| double | deltaGammaHZZRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.) More... | |
| virtual double | deltaGammaTotalRatio1 () const |
| The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients. More... | |
| virtual double | deltaGammaTotalRatio2 () const |
| The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients. More... | |
| virtual double | DeltaGF () const |
| New physics contribution to the Fermi constant. More... | |
| double | deltaGL_f (const Particle p) const |
| New physics contribution to the neutral-current left-handed coupling \(g_L^f\). More... | |
| virtual gslpp::complex | deltaGL_Wff (const Particle pbar, const Particle p) const |
| New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\). More... | |
| gslpp::complex | deltaGL_Wffh (const Particle pbar, const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_L}\gamma^mu f_L\). More... | |
| double | deltaGL_Zffh (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_L}\gamma^mu f_L\). More... | |
| virtual double | deltaGmu () const |
| The relative correction to the muon decay constant, \(\delta G_\mu/G_\mu\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltaGmu2 () const |
| The relative correction to the muon decay constant, \((\delta G_\mu/G_\mu)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| double | deltaGR_f (const Particle p) const |
| New physics contribution to the neutral-current right-handed coupling \(g_R^f\). More... | |
| virtual gslpp::complex | deltaGR_Wff (const Particle pbar, const Particle p) const |
| New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\). More... | |
| gslpp::complex | deltaGR_Wffh (const Particle pbar, const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_R}\gamma^mu f_R\). More... | |
| double | deltaGR_Zffh (const Particle p) const |
| The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_R}\gamma^mu f_R\). More... | |
| virtual double | deltaGV_f (const Particle p) const |
| New physics contribution to the neutral-current vector coupling \(g_V^f\). More... | |
| virtual double | deltaGwd6 () const |
| The relative NP corrections to the width of the \(W\) boson, \(\delta \Gamma_W/\Gamma_W\). More... | |
| virtual double | deltaGwd62 () const |
| The relative NP corrections to the width of the \(W\) boson squared, \((\delta \Gamma_W/\Gamma_W)^2\). More... | |
| virtual double | deltaGzd6 () const |
| The relative NP corrections to the width of the \(Z\) boson, \(\delta \Gamma_Z/\Gamma_Z\). More... | |
| virtual double | deltaGzd62 () const |
| The relative NP corrections to the width of the \(Z\) boson squared, \((\delta \Gamma_Z/\Gamma_Z)^2\). More... | |
| virtual double | deltaKgammaNP () const |
| The new physics contribution to the anomalous triple gauge coupling \(\kappa_{\gamma}\). More... | |
| virtual double | deltamb () const |
| The relative correction to the mass of the \(b\) quark, \(\delta m_b/m_b\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltamb2 () const |
| The relative correction to the mass of the \(b\) quark squared, \((\delta m_b/m_b)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltamc () const |
| The relative correction to the mass of the \(c\) quark, \(\delta m_c/m_c\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltamc2 () const |
| The relative correction to the mass of the \(c\) quark squared, \((\delta m_c/m_c)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltaMh () const |
| The relative correction to the mass of the \(H\) boson, \(\delta M_H/M_H\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltaMh2 () const |
| The relative correction to the mass of the \(H\) boson squared, \((\delta M_H/M_H)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltamt () const |
| The relative correction to the mass of the \(t\) quark, \(\delta m_t/m_t\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltamt2 () const |
| The relative correction to the mass of the \(t\) quark squared, \((\delta m_t/m_t)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltamtau () const |
| The relative correction to the mass of the \(\tau\) lepton, \(\delta m_\tau/m_\tau\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltamtau2 () const |
| The relative correction to the mass of the \(\tau\) lepton squared, \((\delta m_\tau/m_\tau)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltaMwd6 () const |
| The relative NP corrections to the mass of the \(W\) boson, \(\delta M_W/M_W\). More... | |
| virtual double | deltaMwd62 () const |
| The relative NP corrections to the mass of the \(W\) boson squared, \((\delta M_W/M_W)^2\). More... | |
| virtual double | deltaMz () const |
| The relative correction to the mass of the \(Z\) boson, \(\delta M_Z/M_Z\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltaMz2 () const |
| The relative correction to the mass of the \(Z\) boson squared, \((\delta M_Z/M_Z)^2\), with respect to ref. point used in the SM calculation of Higgs observables. More... | |
| virtual double | deltayb_HB () const |
| The Higgs-basis coupling \(\delta y_b\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | deltayc_HB () const |
| The Higgs-basis coupling \(\delta y_c\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | deltaymu_HB () const |
| The Higgs-basis coupling \(\delta y_\mu\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | deltayt_HB () const |
| The Higgs-basis coupling \(\delta y_t\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | deltaytau_HB () const |
| The Higgs-basis coupling \(\delta y_\tau\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | dxseeWWdcos (const double sqrt_s, const double cos) const |
| The differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\), as a function of the \(W\) polar angle. More... | |
| virtual double | dxseeWWdcosBin (const double sqrt_s, const double cos1, const double cos2) const |
| The integral of differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\) in a given bin of the \(W\) polar angle. More... | |
| gslpp::complex | f_triangle (const double tau) const |
| Loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings. More... | |
| gslpp::complex | g_triangle (const double tau) const |
| Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| double | GammaHbbRatio () const |
| The ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. More... | |
| double | GammaHccRatio () const |
| The ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. More... | |
| double | GammaHgagaRatio () const |
| The ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. More... | |
| double | GammaHggRatio () const |
| The ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. More... | |
| double | GammaHmumuRatio () const |
| The ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. More... | |
| double | GammaHtautauRatio () const |
| The ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. More... | |
| double | GammaHWffRatio () const |
| The ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| double | GammaHWjjRatio () const |
| The ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. More... | |
| double | GammaHWlvRatio () const |
| The ratio of the \(\Gamma(H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| double | GammaHWW2l2vRatio () const |
| The ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| double | GammaHWW4fRatio () const |
| The ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| double | GammaHWW4jRatio () const |
| The ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. More... | |
| double | GammaHWWRatio () const |
| The ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. More... | |
| double | GammaHZddRatio () const |
| The ratio of the \(\Gamma(H\to Zd d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More... | |
| double | GammaHZeeRatio () const |
| The ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. More... | |
| double | GammaHZffRatio () const |
| The ratio of the \(\Gamma(H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| double | GammaHZgaRatio () const |
| The ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. More... | |
| double | GammaHZllRatio () const |
| The ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| double | GammaHZmumuRatio () const |
| The ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. More... | |
| double | GammaHZuuRatio () const |
| The ratio of the \(\Gamma(H\to Zu u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More... | |
| double | GammaHZvvRatio () const |
| The ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. More... | |
| double | GammaHZZ2e2muRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. More... | |
| double | GammaHZZ4dRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. More... | |
| double | GammaHZZ4eRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. More... | |
| double | GammaHZZ4fRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. More... | |
| double | GammaHZZ4lRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. More... | |
| double | GammaHZZ4muRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. More... | |
| double | GammaHZZ4uRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. More... | |
| double | GammaHZZ4vRatio () const |
| The ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. More... | |
| double | GammaHZZRatio () const |
| The ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. More... | |
| virtual double | GammaW (const Particle fi, const Particle fj) const |
| A partial decay width of the \(W\) boson decay into a SM fermion pair. More... | |
| virtual double | GammaW () const |
| The total width of the \(W\) boson, \(\Gamma_W\). More... | |
| double | getCed_1123 () const |
| Return NP coeff Ced_1123. More... | |
| double | getCed_2223 () const |
| Return NP coeff Ced_2223. More... | |
| double | getCeu_1133 () const |
| Return NP coeff Ceu_1133. More... | |
| double | getCeu_2233 () const |
| Return NP coeff Ceu_2233. More... | |
| double | getCHe_11 () const |
| Return NP coeff CHe_11. More... | |
| double | getCHe_22 () const |
| Return NP coeff CHe_22. More... | |
| double | getCHL1_11 () const |
| Return NP coeff CHL1_11. More... | |
| double | getCHL1_22 () const |
| Return NP coeff CHL1_22. More... | |
| double | getCHL3_11 () const |
| Return NP coeff CHL3_11. More... | |
| double | getCHL3_22 () const |
| Return NP coeff CHL3_22. More... | |
| double | getCLd_1123 () const |
| Return NP coeff CLd_1123. More... | |
| double | getCLd_2223 () const |
| Return NP coeff CLd_2223. More... | |
| double | getCLedQ_11 () const |
| Return NP coeff CLedq_11. More... | |
| double | getCLedQ_22 () const |
| Return NP coeff CLedq_22. More... | |
| double | getCLQ1_1123 () const |
| Return NP coeff CLQ1_1123. More... | |
| double | getCLQ1_2223 () const |
| Return NP coeff CLQ1_2223. More... | |
| double | getCLQ3_1123 () const |
| Return NP coeff CLQ3_1123. More... | |
| double | getCLQ3_2223 () const |
| Return NP coeff CLQ3_2223. More... | |
| double | getCLu_1133 () const |
| Return NP coeff CLu_1133. More... | |
| double | getCLu_2233 () const |
| Return NP coeff CLu_2233. More... | |
| double | getCpLedQ_11 () const |
| Return NP coeff CpLedq_11. More... | |
| double | getCpLedQ_22 () const |
| Return NP coeff CpLedq_22. More... | |
| double | getCQe_2311 () const |
| Return NP coeff CQe_2322. More... | |
| double | getCQe_2322 () const |
| Return NP coeff CQe_2322. More... | |
| double | getLambda_NP () const |
| Return Lambda_NP. More... | |
| virtual NPSMEFTd6Matching & | getMatching () const |
| A method to get the Matching object for this model. More... | |
| gslpp::complex | I_triangle_1 (const double tau, const double lambda) const |
| Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| gslpp::complex | I_triangle_2 (const double tau, const double lambda) const |
| Loop function entering in the calculation of the effective \(HZ\gamma\) coupling. More... | |
| virtual double | kappaAeff () const |
| The effective coupling \(\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}\). More... | |
| virtual double | kappabeff () const |
| The effective coupling \(\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}\). More... | |
| virtual double | kappaceff () const |
| The effective coupling \(\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}\). More... | |
| virtual double | kappaGeff () const |
| The effective coupling \(\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}\). More... | |
| virtual double | kappamueff () const |
| The effective coupling \(\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}\). More... | |
| virtual double | kappataueff () const |
| The effective coupling \(\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}\). More... | |
| virtual double | kappaWeff () const |
| The effective coupling \(\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}\). More... | |
| virtual double | kappaZAeff () const |
| The effective coupling \(\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}\). More... | |
| virtual double | kappaZeff () const |
| The effective coupling \(\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}\). More... | |
| virtual double | lambdaZNP () const |
| The new physics contribution to the anomalous triple gauge coupling \(\lambda_{Z}\). More... | |
| virtual double | lambz_HB () const |
| The Higgs-basis coupling \(\lambda_{z}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\). More... | |
| virtual double | mueeHvv (const double sqrt_s) const |
| The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeHvvPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueettH (const double sqrt_s) const |
| The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueettHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeWBF (const double sqrt_s) const |
| The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeWBFPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeZBF (const double sqrt_s) const |
| The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeZBFPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeZH (const double sqrt_s) const |
| The ratio \(\mu_{eeZH}\) between the \(e^{+}e^{-}\to ZH\) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeZHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeZllH (const double sqrt_s) const |
| The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeZllHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeZqqH (const double sqrt_s) const |
| The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mueeZqqHPol (const double sqrt_s, const double Pol_em, const double Pol_ep) const |
| The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muepWBF (const double sqrt_s) const |
| The ratio \(\mu_{epWBF}\) between the \( e^{-} p\to \nu j H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muepZBF (const double sqrt_s) const |
| The ratio \(\mu_{epZBF}\) between the \( e^{-} p\to e^{-} j H \) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muggH (const double sqrt_s) const |
| The ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muggHbb (const double sqrt_s) const |
| The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual double | muggHgaga (const double sqrt_s) const |
| The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual double | muggHH (const double sqrt_s) const |
| The ratio \(\mu_{ggHH}\) between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model. (From arXiv: 1502.00539 [hpe-ph].) More... | |
| virtual double | muggHmumu (const double sqrt_s) const |
| The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual double | muggHpttH (const double sqrt_s) const |
| The ratio \(\mu_{ggH+ttH}\) between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muggHtautau (const double sqrt_s) const |
| The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual double | muggHWW (const double sqrt_s) const |
| The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual double | muggHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual double | muggHZga (const double sqrt_s) const |
| The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual double | muggHZZ (const double sqrt_s) const |
| The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual double | muggHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual double | mummH (const double sqrt_s) const |
| The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model. More... | |
| virtual double | mupTVppWZ (const double sqrt_s, const double pTV1, const double pTV2) const |
| The number of events in \( p p \to WZ\) in a given \(p_{TV}\) bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6 class. More... | |
| virtual double | muttH (const double sqrt_s) const |
| The ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muttHbb (const double sqrt_s) const |
| The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual double | muttHgaga (const double sqrt_s) const |
| The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual double | muttHmumu (const double sqrt_s) const |
| The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual double | muttHtautau (const double sqrt_s) const |
| The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual double | muttHWW (const double sqrt_s) const |
| The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual double | muttHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual double | muttHZbbboost (const double sqrt_s) const |
| The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H,Z\to b\bar{b}\) channel in the current model and in the Standard Model. More... | |
| virtual double | muttHZga (const double sqrt_s) const |
| The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual double | muttHZZ (const double sqrt_s) const |
| The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual double | muttHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual double | muVBF (const double sqrt_s) const |
| The ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muVBFgamma (const double sqrt_s) const |
| The ratio \(\mu_{VBF+\gamma}\) between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model. More... | |
| virtual double | muVBFHbb (const double sqrt_s) const |
| The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual double | muVBFHgaga (const double sqrt_s) const |
| The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual double | muVBFHmumu (const double sqrt_s) const |
| The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual double | muVBFHtautau (const double sqrt_s) const |
| The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual double | muVBFHWW (const double sqrt_s) const |
| The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual double | muVBFHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual double | muVBFHZga (const double sqrt_s) const |
| The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual double | muVBFHZZ (const double sqrt_s) const |
| The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual double | muVBFHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual double | muVBFpVH (const double sqrt_s) const |
| The ratio \(\mu_{VBF+VH}\) between the sum of VBF and WH+ZH associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muVH (const double sqrt_s) const |
| The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muVHbb (const double sqrt_s) const |
| The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual double | muVHgaga (const double sqrt_s) const |
| The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual double | muVHmumu (const double sqrt_s) const |
| The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual double | muVHtautau (const double sqrt_s) const |
| The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual double | muVHWW (const double sqrt_s) const |
| The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual double | muVHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual double | muVHZga (const double sqrt_s) const |
| The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual double | muVHZZ (const double sqrt_s) const |
| The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual double | muVHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual double | muWH (const double sqrt_s) const |
| The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muWHbb (const double sqrt_s) const |
| The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual double | muWHgaga (const double sqrt_s) const |
| The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual double | muWHmumu (const double sqrt_s) const |
| The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual double | muWHtautau (const double sqrt_s) const |
| The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual double | muWHWW (const double sqrt_s) const |
| The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual double | muWHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual double | muWHZga (const double sqrt_s) const |
| The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual double | muWHZZ (const double sqrt_s) const |
| The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual double | muWHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual double | muZH (const double sqrt_s) const |
| The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model. More... | |
| virtual double | muZHbb (const double sqrt_s) const |
| The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model. More... | |
| virtual double | muZHgaga (const double sqrt_s) const |
| The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. More... | |
| virtual double | muZHmumu (const double sqrt_s) const |
| The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model. More... | |
| virtual double | muZHtautau (const double sqrt_s) const |
| The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model. More... | |
| virtual double | muZHWW (const double sqrt_s) const |
| The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model. More... | |
| virtual double | muZHWW2l2v (const double sqrt_s) const |
| The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model. More... | |
| virtual double | muZHZga (const double sqrt_s) const |
| The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model. More... | |
| virtual double | muZHZZ (const double sqrt_s) const |
| The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model. More... | |
| virtual double | muZHZZ4l (const double sqrt_s) const |
| The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model. More... | |
| virtual double | Mw () const |
| The mass of the \(W\) boson, \(M_W\). More... | |
| NPSMEFTd6 (const bool FlagLeptonUniversal_in=false, const bool FlagQuarkUniversal_in=false) | |
| Constructor. More... | |
| virtual double | obliqueS () const |
| The oblique parameter \(S\). (Simplified implementation. Contribution only from \(O_{HWB}\).) More... | |
| virtual double | obliqueT () const |
| The oblique parameter \(T\). (Simplified implementation. Contribution only from \(O_{HD}\).) More... | |
| virtual double | obliqueU () const |
| The oblique parameter \(U\). More... | |
| virtual double | obliqueW () const |
| The oblique parameter \(W\). (Simplified implementation. Contribution only from \(O_{2W}\).) More... | |
| virtual double | obliqueY () const |
| The oblique parameter \(Y\). (Simplified implementation. Contribution only from \(O_{2B}\).) More... | |
| virtual bool | PostUpdate () |
| The post-update method for NPSMEFTd6. More... | |
| virtual double | ppZHprobe (const double sqrt_s) const |
| The direction constrained by \( p p \to Z H\) in the boosted regime, \(g_p^Z\). From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6 class. More... | |
| virtual bool | setFlag (const std::string name, const bool value) |
| A method to set a flag of NPSMEFTd6. More... | |
| virtual double | xseeWW (const double sqrt_s) const |
| Total \(e^+ e^- \to W^+ W^- \to jj \ell \nu\) cross section in pb, with \(\ell= e, \mu\). More... | |
 Public Member Functions inherited from NPbase | |
| virtual double | A_f (const Particle f) const |
| The left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\mathcal{A}_f\). More... | |
| virtual double | AFB (const Particle f) const |
| The forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(A^f_{FB}\). More... | |
| virtual double | BR_Zf (const Particle f) const |
| The Branching ratio of the \(Z\) boson into a given fermion pair, \(BR_Z^{f}\). More... | |
| virtual double | cbminuscc () const |
| virtual double | cbminusctau () const |
| virtual double | ccminusctau () const |
| virtual double | cgaplusct () const |
| virtual double | cgminuscga () const |
| virtual double | cgplusct () const |
| virtual double | cVpluscb () const |
| virtual double | cVplusctau () const |
| virtual double | deltaA_f (const Particle f) const |
| The new physics contribution to the left-right asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta \mathcal{A}_f\). More... | |
| virtual double | deltaAFB (const Particle f) const |
| The new physics contribution to the forward-backward asymmetry in \(e^+e^-\to Z\to f \bar{f}\) at the \(Z\)-pole, \(\delta A^f_{FB}\). More... | |
| virtual double | deltaGamma_Z () const |
| The new physics contribution to the total decay width of the \(Z\) boson, \(\delta \Gamma_Z\). More... | |
| virtual double | deltaGamma_Zf (const Particle f) const |
| The new physics contribution to the decay width of the \(Z\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\). More... | |
| virtual double | deltaN_nu () const |
| The new physics contribution to the number of neutrinos dervied from the \(Z\) pole measurements. More... | |
| virtual double | deltaR0_f (const Particle f) const |
| The new physics contribution to the ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\) or \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\), for leptons or quarks, respectively. More... | |
| virtual double | deltaR_inv () const |
| The new physics contribution to the ratio of invisible and leptonic (electron) decay widths of the \(Z\) boson, \(\delta R_{inv}\). More... | |
| virtual double | deltaSigmaHadron () const |
| The new physics contribution to the cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\delta \sigma_h^0\). More... | |
| virtual double | deltaSin2thetaEff_e () const |
| The new physics contribution to the effective electron/leptonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\rm lept}\) at the \(Z\) pole. More... | |
| virtual double | deltaSin2thetaEff_mu () const |
| The new physics contribution to the effective muonic weak angle \(\delta \sin^2\theta_{\rm eff}^{\mu\mu}\) at the \(Z\) pole. More... | |
| virtual gslpp::complex | gA_f (const Particle f) const |
| The total (SM+NP) contribution to the neutral-current axial-vector coupling \(g_A^f\). More... | |
| virtual double | Gamma_Z () const |
| The total decay width of the \(Z\) boson, \(\Gamma_Z\). More... | |
| virtual double | Gamma_Zf (const Particle f) const |
| The decay width of the \(Z\) boson into a given fermion pair, \(\Gamma_Z^{f}\). More... | |
| virtual StandardModel | getTrueSM () const |
| A method to return a StandardModel object from NPbase. More... | |
| virtual gslpp::complex | gV_f (const Particle f) const |
| The total (SM+NP) contribution to the neutral-current vector coupling \(g_V^f\). More... | |
| virtual gslpp::complex | kappaZ_f (const Particle f) const |
| The effective neutral-current coupling \(\kappa_Z^f\) including SM plus NP contributions. More... | |
| virtual double | muggHgagaInt (const double sqrt_s) const |
| The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model. Includes interference effects with the background, following arXiv:1704.08259. More... | |
| virtual double | muppHmumu (const double sqrt_s) const |
| virtual double | muppHZga (const double sqrt_s) const |
| virtual double | N_nu () const |
| The number of neutrinos dervied from the \(Z\) pole measurements, \(N_{\nu}\). More... | |
| NPbase () | |
| The default constructor. More... | |
| virtual double | R0_f (const Particle f) const |
| The ratio \(R_\ell^0=\Gamma_{\mathrm{had}}/\Gamma_\ell\) or \(R_q^0=\Gamma_q/\Gamma_{\mathrm{had}}\), for leptons or quarks, respectively. More... | |
| virtual double | R_inv () const |
| The ratio of the invisible and leptonic (electron) decay widths of the \(Z\) boson, \(R_{inv}\). More... | |
| virtual gslpp::complex | rhoZ_f (const Particle f) const |
| The effective neutral-current coupling \(\rho_Z^f\) including SM plus NP contributions. More... | |
| virtual double | sigma0_had () const |
| The cross section for the process \(e^+ e^-\to Z\to \mathrm{hadrons}\) at the \(Z\) pole, \(\sigma_h^0\). More... | |
| virtual double | sin2thetaEff (const Particle f) const |
| The leptonic effective weak mixing angle \(\sin^2\theta_{\rm eff}^{\rm lept}\) at the the \(Z\) pole. More... | |
| virtual bool | Update (const std::map< std::string, double > &DPars) |
| The update method for NPbase. More... | |
| virtual double | UpperLimitZgammaA (const double sqrt_s) const |
| virtual double | UpperLimitZgammaA13 (const double sqrt_s) const |
| virtual double | UpperLimitZgammaC (const double sqrt_s) const |
| virtual double | UpperLimitZgammaC13 (const double sqrt_s) const |
| Public Member Functions inherited from StandardModel | |
| double | Ale (double mu, orders order, bool Nf_thr=true) const |
| The running electromagnetic coupling \(\alpha_e(\mu)\) in the \(\overline{MS}\) scheme. More... | |
| double | ale_OS (const double mu, orders order=FULLNLO) const |
| The running electromagnetic coupling \(\alpha(\mu)\) in the on-shell scheme. More... | |
| double | alphaMz () const |
| The electromagnetic coupling at the \(Z\)-mass scale, \(\alpha(M_Z^2)=\alpha/(1-\Delta\alpha(M_Z^2))\). More... | |
| double | Als (double mu, orders order=FULLNLO, bool qed_flag=false, bool Nf_thr=true) const |
| The running QCD coupling \(\alpha(\mu)\) in the \(\overline{MS}\) scheme including QED corrections. More... | |
| double | AlsByOrder (double mu, orders order=FULLNLO, bool qed_flag=false, bool Nf_thr=true) const |
| double | Beta_e (int nm, unsigned int nf) const |
| QED beta function coefficients - eq. (36) hep-ph/0512066. More... | |
| double | Beta_s (int nm, unsigned int nf) const |
| QCD beta function coefficients including QED corrections - eq. (36) hep-ph/0512066. More... | |
| double | c02 () const |
| The square of the cosine of the weak mixing angle \(c_0^2\) defined without weak radiative corrections. More... | |
| virtual bool | CheckFlags () const |
| A method to check the sanity of the set of model flags. More... | |
| bool | checkSMparamsForEWPO () |
| A method to check whether the parameters relevant to the EWPO are updated. More... | |
| double | computeBrHtobb () const |
| The Br \((H\to bb)\) in the Standard Model. More... | |
| double | computeBrHtocc () const |
| The Br \((H\to cc)\) in the Standard Model. More... | |
| double | computeBrHtogaga () const |
| The Br \((H\to\gamma\gamma)\) in the Standard Model. More... | |
| double | computeBrHtogg () const |
| The Br \((H\to gg)\) in the Standard Model. More... | |
| double | computeBrHtomumu () const |
| The Br \((H\to \mu\mu)\) in the Standard Model. More... | |
| double | computeBrHtotautau () const |
| The Br \((H\to \tau\tau)\) in the Standard Model. More... | |
| double | computeBrHtoWW () const |
| The Br \((H\to WW)\) in the Standard Model. More... | |
| double | computeBrHtoZga () const |
| The Br \((H\to Z\gamma)\) in the Standard Model. More... | |
| double | computeBrHtoZZ () const |
| The Br \((H\to ZZ)\) in the Standard Model. More... | |
| double | computeBrHtoZZinv () const |
| The Br \((H\to ZZ \to inv)\) in the Standard Model. More... | |
| void | ComputeDeltaR_rem (const double Mw_i, double DeltaR_rem[orders_EW_size]) const |
| A method to collect \(\Delta r_{\mathrm{rem}}\) computed via subclasses. More... | |
| void | ComputeDeltaRho (const double Mw_i, double DeltaRho[orders_EW_size]) const |
| A method to collect \(\Delta\rho\) computed via subclasses. More... | |
| double | computeGammaHgaga_tt () const |
| The top loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More... | |
| double | computeGammaHgaga_tW () const |
| The mixed \(t-W\) loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More... | |
| double | computeGammaHgaga_WW () const |
| The \(W\) loop contribution to \(H\to\gamma\gamma\) in the Standard Model. More... | |
| double | computeGammaHgg_bb () const |
| The bottom loop contribution to \(H\to gg\) in the Standard Model. More... | |
| double | computeGammaHgg_tb () const |
| The top-bottom interference contribution to \(H\to gg\) in the Standard Model. More... | |
| double | computeGammaHgg_tt () const |
| The top loop contribution to \(H\to gg\) in the Standard Model. More... | |
| double | computeGammaHTotal () const |
| The Higgs total width in the Standard Model. More... | |
| double | computeGammaHZga_tt () const |
| The top loop contribution to \(H\to Z\gamma\) in the Standard Model. More... | |
| double | computeGammaHZga_tW () const |
| The mixed \(t-W\) loop contribution to \(H\to Z\gamma\) in the Standard Model. More... | |
| double | computeGammaHZga_WW () const |
| The \(W\) loop contribution to \(H\to Z\gamma\) in the Standard Model. Currently it returns the value of tab 41 in ref. [94]. More... | |
| double | computeSigmaggH (const double sqrt_s) const |
| The ggH cross section in the Standard Model. More... | |
| double | computeSigmaggH_bb (const double sqrt_s) const |
| The square of the bottom-quark contribution to the ggH cross section in the Standard Model. More... | |
| double | computeSigmaggH_tb (const double sqrt_s) const |
| The top-bottom interference contribution to the ggH cross section in the Standard Model. More... | |
| double | computeSigmaggH_tt (const double sqrt_s) const |
| The square of the top-quark contribution to the ggH cross section in the Standard Model. More... | |
| double | computeSigmattH (const double sqrt_s) const |
| The ttH production cross section in the Standard Model. More... | |
| double | computeSigmaVBF (const double sqrt_s) const |
| The VBF cross section in the Standard Model. More... | |
| double | computeSigmaWF (const double sqrt_s) const |
| The W fusion contribution \(\sigma_{WF}\) to higgs-production cross section in the Standard Model. More... | |
| double | computeSigmaWH (const double sqrt_s) const |
| The WH production cross section in the Standard Model. More... | |
| double | computeSigmaZF (const double sqrt_s) const |
| The Z fusion contribution \(\sigma_{ZF}\) to higgs-production cross section in the Standard Model. More... | |
| double | computeSigmaZH (const double sqrt_s) const |
| The ZH production cross section in the Standard Model. More... | |
| double | computeSigmaZWF (const double sqrt_s) const |
| The Z W interference fusion contribution \(\sigma_{ZWF}\) to higgs-production cross section in the Standard Model. More... | |
| virtual double | cW2 (const double Mw_i) const |
| The square of the cosine of the weak mixing angle in the on-shell scheme, denoted as \(c_W^2\). More... | |
| virtual double | cW2 () const |
| double | DeltaAlpha () const |
| The total corrections to the electromagnetic coupling \(\alpha\) at the \(Z\)-mass scale, denoted as \(\Delta\alpha(M_Z^2)\). More... | |
| double | DeltaAlphaL5q () const |
| The sum of the leptonic and the five-flavour hadronic corrections to the electromagnetic coupling \(\alpha\) at the \(Z\)-mass scale, denoted as \(\Delta\alpha^{\ell+5q}(M_Z^2)\). More... | |
| double | DeltaAlphaLepton (const double s) const |
| Leptonic contribution to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{lept}}(s)\). More... | |
| double | DeltaAlphaTop (const double s) const |
| Top-quark contribution to the electromagnetic coupling \(\alpha\), denoted as \(\Delta\alpha_{\mathrm{top}}(s)\). More... | |
| virtual gslpp::complex | deltaKappaZ_f (const Particle f) const |
| Flavour non-universal vertex corrections to \(\kappa_Z^l\), denoted by \(\Delta\kappa_Z^l\). More... | |
| virtual double | DeltaR () const |
| The SM prediction for \(\Delta r\) derived from that for the \(W\) boson mass. More... | |
| virtual double | DeltaRbar () const |
| The SM prediction for \(\Delta \overline{r}\) derived from that for the \(W\)-boson mass. More... | |
| virtual gslpp::complex | deltaRhoZ_f (const Particle f) const |
| Flavour non-universal vertex corrections to \(\rho_Z^l\), denoted by \(\Delta\rho_Z^l\). More... | |
| virtual double | epsilon1 () const |
| The SM contribution to the epsilon parameter \(\varepsilon_1\). More... | |
| virtual double | epsilon2 () const |
| The SM contribution to the epsilon parameter \(\varepsilon_2\). More... | |
| virtual double | epsilon3 () const |
| The SM contribution to the epsilon parameter \(\varepsilon_3\). More... | |
| virtual double | epsilonb () const |
| The SM contribution to the epsilon parameter \(\varepsilon_b\). More... | |
| virtual double | Gamma_had () const |
| The hadronic decay width of the \(Z\) boson, \(\Gamma_{h}\). More... | |
| virtual double | Gamma_inv () const |
| The invisible partial decay width of the \(Z\) boson, \(\Gamma_{\mathrm{inv}}\). More... | |
| virtual double | GammaZ (const Particle f) const |
| The \(Z\to \ell\bar{\ell}\) partial decay width, \(\Gamma_\ell\). More... | |
| double | getAle () const |
| A get method to retrieve the fine-structure constant \(\alpha\). More... | |
| double | getAlsMz () const |
| A get method to access the value of \(\alpha_s(M_Z)\). More... | |
| virtual double | getCBd () const |
| The ratio of the absolute value of the $B_d$ mixing amplitude over the Standard Model value. More... | |
| virtual double | getCBs () const |
| The ratio of the absolute value of the $B_s$ mixing amplitude over the Standard Model value. More... | |
| virtual double | getCDMK () const |
| The ratio of the real part of the $K$ mixing amplitude over the Standard Model value. More... | |
| virtual double | getCepsK () const |
| The ratio of the imaginary part of the $K$ mixing amplitude over the Standard Model value. More... | |
| CKM | getCKM () const |
| A get method to retrieve the member object of type CKM. More... | |
| double | getDAle5Mz () const |
| A get method to retrieve the five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\). More... | |
| double | getDelGammaZ () const |
| A get method to retrieve the theoretical uncertainty in \(\Gamma_Z\), denoted as \(\delta\,\Gamma_Z\). More... | |
| double | getDelMw () const |
| A get method to retrieve the theoretical uncertainty in \(M_W\), denoted as \(\delta\,M_W\). More... | |
| double | getDelR0b () const |
| A get method to retrieve the theoretical uncertainty in \(R_b^0\), denoted as \(\delta\,R_b^0\). More... | |
| double | getDelR0c () const |
| A get method to retrieve the theoretical uncertainty in \(R_c^0\), denoted as \(\delta\,R_c^0\). More... | |
| double | getDelR0l () const |
| A get method to retrieve the theoretical uncertainty in \(R_l^0\), denoted as \(\delta\,R_l^0\). More... | |
| double | getDelSigma0H () const |
| A get method to retrieve the theoretical uncertainty in \(\sigma_{Hadron}^0\), denoted as \(\delta\,\sigma_{Hadron}^0\). More... | |
| double | getDelSin2th_b () const |
| A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{b}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{b}\). More... | |
| double | getDelSin2th_l () const |
| A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{\rm lept}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{\rm lept}\). More... | |
| double | getDelSin2th_q () const |
| A get method to retrieve the theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{q\not = b,t}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{q\not = b,t}\). More... | |
| std::string | getFlagKappaZ () const |
| A method to retrieve the model flag KappaZ. More... | |
| std::string | getFlagMw () const |
| A method to retrieve the model flag Mw. More... | |
| std::string | getFlagRhoZ () const |
| A method to retrieve the model flag RhoZ. More... | |
| const Flavour & | getFlavour () const |
| double | getGF () const |
| A get method to retrieve the Fermi constant \(G_\mu\). More... | |
| int | getIterationNo () const |
| Particle | getLeptons (const QCD::lepton p) const |
| A get method to retrieve the member object of a lepton. More... | |
| virtual double | getMHl () const |
| A get method to retrieve the Higgs mass \(m_h\). More... | |
| virtual double | getmq (const QCD::quark q, const double mu) const |
| double | getMuw () const |
| A get method to retrieve the matching scale \(\mu_W\) around the weak scale. More... | |
| EWSMApproximateFormulae * | getMyApproximateFormulae () const |
| A get method to retrieve the member pointer of type EWSMApproximateFormulae. More... | |
| EWSMcache * | getMyEWSMcache () const |
| A get method to retrieve the member pointer of type EWSMcache. More... | |
| LeptonFlavour * | getMyLeptonFlavour () const |
| EWSMOneLoopEW * | getMyOneLoopEW () const |
| A get method to retrieve the member pointer of type EWSMOneLoopEW,. More... | |
| EWSMThreeLoopEW * | getMyThreeLoopEW () const |
| EWSMThreeLoopEW2QCD * | getMyThreeLoopEW2QCD () const |
| EWSMThreeLoopQCD * | getMyThreeLoopQCD () const |
| EWSMTwoFermionsLEP2 * | getMyTwoFermionsLEP2 () const |
| A get method to retrieve the member pointer of type EWSMTwoFermionsLEP2. More... | |
| EWSMTwoLoopEW * | getMyTwoLoopEW () const |
| EWSMTwoLoopQCD * | getMyTwoLoopQCD () const |
| double | getMz () const |
| A get method to access the mass of the \(Z\) boson \(M_Z\). More... | |
| virtual double | getPhiBd () const |
| Half the relative phase of the $B_d$ mixing amplitude w.r.t. the Standard Model one. More... | |
| virtual double | getPhiBs () const |
| Half the relative phase of the $B_s$ mixing amplitude w.r.t. the Standard Model one. More... | |
| gslpp::matrix< gslpp::complex > | getUPMNS () const |
| A get method to retrieve the object of the PMNS matrix. More... | |
| gslpp::matrix< gslpp::complex > | getVCKM () const |
| A get method to retrieve the CKM matrix. More... | |
| gslpp::matrix< gslpp::complex > | getYd () const |
| A get method to retrieve the Yukawa matrix of the down-type quarks, \(Y_d\). More... | |
| gslpp::matrix< gslpp::complex > | getYe () const |
| A get method to retrieve the Yukawa matrix of the charged leptons, \(Y_e\). More... | |
| gslpp::matrix< gslpp::complex > | getYn () const |
| A get method to retrieve the Yukawa matrix of the neutrinos, \(Y_\nu\). More... | |
| gslpp::matrix< gslpp::complex > | getYu () const |
| A get method to retrieve the Yukawa matrix of the up-type quarks, \(Y_u\). More... | |
| virtual bool | Init (const std::map< std::string, double > &DPars) |
| A method to initialize the model parameters. More... | |
| virtual bool | InitializeModel () |
| A method to initialize the model. More... | |
| bool | IsFlagNoApproximateGammaZ () const |
| A method to retrieve the model flag NoApproximateGammaZ. More... | |
| bool | IsFlagWithoutNonUniversalVC () const |
| A method to retrieve the model flag WithoutNonUniversalVC. More... | |
| virtual double | LEP2AFBbottom (const double s) const |
| virtual double | LEP2AFBcharm (const double s) const |
| virtual double | LEP2AFBmu (const double s) const |
| virtual double | LEP2AFBtau (const double s) const |
| virtual double | LEP2Rbottom (const double s) const |
| virtual double | LEP2Rcharm (const double s) const |
| virtual double | LEP2sigmaBottom (const double s) const |
| virtual double | LEP2sigmaCharm (const double s) const |
| virtual double | LEP2sigmaHadron (const double s) const |
| virtual double | LEP2sigmaMu (const double s) const |
| virtual double | LEP2sigmaTau (const double s) const |
| virtual double | Mw_tree () const |
| The tree-level mass of the \(W\) boson, \(M_W^{\mathrm{tree}}\). More... | |
| double | MwbarFromMw (const double Mw) const |
| A method to convert the \(W\)-boson mass in the experimental/running-width scheme to that in the complex-pole/fixed-width scheme. More... | |
| double | MwFromMwbar (const double Mwbar) const |
| A method to convert the \(W\)-boson mass in the complex-pole/fixed-width scheme to that in the experimental/running-width scheme. More... | |
| double | Mzbar () const |
| The \(Z\)-boson mass \(\overline{M}_Z\) in the complex-pole/fixed-width scheme. More... | |
| virtual bool | PreUpdate () |
| The pre-update method for StandardModel. More... | |
| virtual double | rho_GammaW (const Particle fi, const Particle fj) const |
| EW radiative corrections to the width of \(W \to f_i \bar{f}_j\), denoted as \(\rho^W_{ij}\). More... | |
| double | s02 () const |
| The square of the sine of the weak mixing angle \(s_0^2\) defined without weak radiative corrections. More... | |
| void | setFlagCacheInStandardModel (bool FlagCacheInStandardModel) |
| A set method to change the model flag CacheInStandardModel of StandardModel. More... | |
| void | setFlagNoApproximateGammaZ (bool FlagNoApproximateGammaZ) |
| bool | setFlagSigmaForAFB (const bool flagSigmaForAFB_i) |
| bool | setFlagSigmaForR (const bool flagSigmaForR_i) |
| virtual bool | setFlagStr (const std::string name, const std::string value) |
| A method to set a flag of StandardModel. More... | |
| StandardModel () | |
| The default constructor. More... | |
| virtual double | sW2 (const double Mw_i) const |
| The square of the sine of the weak mixing angle in the on-shell scheme, denoted as \(s_W^2\). More... | |
| double | sW2 () const |
| virtual double | v () const |
| The value of \(\frac{\alpha_s^{\mathrm{FULLNLO}}}{4\pi}\) at any scale \(\mu\) with the number of flavours \(n_f = 4\) and full EW corrections. More... | |
| virtual | ~StandardModel () |
| The default destructor. More... | |
| Public Member Functions inherited from QCD | |
| double | AboveTh (const double mu) const |
| The active flavour threshold above the scale \(\mu\) as defined in QCD::Thresholds(). More... | |
| void | addParameters (std::vector< std::string > params_i) |
| A method to add parameters that are specific to only one set of observables. More... | |
| virtual double | Als (const double mu, const orders order=FULLNLO, bool Nf_thr=true) const |
| double | Als4 (const double mu) const |
| The value of \(\alpha_s^{\mathrm{FULLNLO}}\) at any scale \(\mu\) with the number of flavours \(n_f = 4\). More... | |
| virtual double | AlsByOrder (const double mu, const orders order=FULLNLO, bool Nf_thr=true) const |
| double | AlsOLD (const double mu, const orders order=FULLNLO) const |
| Computes the running strong coupling \(\alpha_s(\mu)\) in the \(\overline{\mathrm{MS}}\) scheme. In the cases of LO, NLO and FULLNNLO, the coupling is computed with AlsWithInit(). On the other hand, in the cases of NNLO and FULLNNLO, the coupling is computed with AlsWithLambda(). More... | |
| double | AlsWithInit (const double mu, const double alsi, const double mu_i, const orders order) const |
| Computes the running strong coupling \(\alpha_s(\mu)\) from \(\alpha_s(\mu_i)\) in the \(\overline{\mathrm{MS}}\) scheme, where it is forbidden to across a flavour threshold in the RG running from \(\mu_i\) to \(\mu\). More... | |
| double | AlsWithLambda (const double mu, const orders order) const |
| Computes the running strong coupling \(\alpha_s(\mu)\) in the \(\overline{\mathrm{MS}}\) scheme with the use of \(\Lambda_{\rm QCD}\). More... | |
| double | BelowTh (const double mu) const |
| The active flavour threshold below the scale \(\mu\) as defined in QCD::Thresholds(). More... | |
| double | Beta0 (const double nf) const |
| The \(\beta_0(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| double | Beta1 (const double nf) const |
| The \(\beta_1(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| double | Beta2 (const double nf) const |
| The \(\beta_2(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| double | Beta3 (const double nf) const |
| The \(\beta_3(n_f)\) coefficient for a certain number of flavours \(n_f\). More... | |
| void | CacheShift (double cache[][5], int n) const |
| A member used to manage the caching for this class. More... | |
| void | CacheShift (int cache[][5], int n) const |
| orders | FullOrder (orders order) const |
| Return the FULLORDER enum corresponding to order. More... | |
| double | Gamma0 (const double nf) const |
| The \(\gamma_0\) coefficient used to compute the running of a mass. More... | |
| double | Gamma1 (const double nf) const |
| The \(\gamma_1\) coefficient used to compute the running of a mass. More... | |
| double | Gamma2 (const double nf) const |
| The \(\gamma_2\) coefficient used to compute the running of a mass. More... | |
| double | getAlsM () const |
| A get method to access the value of \(\alpha_s(M_{\alpha_s})\). More... | |
| BParameter | getBBd () const |
| For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta b = 2\) process in the \(B_d\) meson system. More... | |
| BParameter | getBBs () const |
| For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta b = 2\) process in the \(B_s\) meson system. More... | |
| BParameter | getBD () const |
| For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta c = 2\) process in the \(D^0\) meson system. More... | |
| BParameter | getBK () const |
| For getting the bag parameters corresponding to the operator basis \(O_1 -O_5\) in \(\Delta s = 2\) process in the \(K^0\) meson system. More... | |
| BParameter | getBKd1 () const |
| BParameter | getBKd3 () const |
| double | getCF () const |
| A get method to access the Casimir factor of QCD. More... | |
| double | getMAls () const |
| A get method to access the mass scale \(M_{\alpha_s}\) at which the strong coupling constant measurement is provided. More... | |
| Meson | getMesons (const QCD::meson m) const |
| A get method to access a meson as an object of the type Meson. More... | |
| double | getMtpole () const |
| A get method to access the pole mass of the top quark. More... | |
| double | getMub () const |
| A get method to access the threshold between five- and four-flavour theory in GeV. More... | |
| double | getMuc () const |
| A get method to access the threshold between four- and three-flavour theory in GeV. More... | |
| double | getMut () const |
| A get method to access the threshold between six- and five-flavour theory in GeV. More... | |
| double | getNc () const |
| A get method to access the number of colours \(N_c\). More... | |
| double | getOptionalParameter (std::string name) const |
| A method to get parameters that are specific to only one set of observables. More... | |
| Particle | getQuarks (const QCD::quark q) const |
| A get method to access a quark as an object of the type Particle. More... | |
| std::vector< std::string > | getUnknownParameters () |
| A method to get the vector of the parameters that have been specified in the configuration file but not being used. More... | |
| void | initializeBParameter (std::string name_i) const |
| A method to initialize B Parameter and the corresponding meson. More... | |
| void | initializeMeson (QCD::meson meson_i) const |
| A method to initialize a meson. More... | |
| double | logLambda (const double nf, orders order) const |
| Computes \(\ln\Lambda_\mathrm{QCD}\) with nf flavours in GeV. More... | |
| double | Mbar2Mp (const double mbar, const orders order=FULLNLO) const |
| Converts the \(\overline{\mathrm{MS}}\) mass \(m(m)\) to the pole mass. More... | |
| double | Mp2Mbar (const double mp, const orders order=FULLNLO) const |
| Converts a quark pole mass to the corresponding \(\overline{\mathrm{MS}}\) mass \(m(m)\). More... | |
| double | Mrun (const double mu, const double m, const orders order=FULLNLO) const |
| Computes a running quark mass \(m(\mu)\) from \(m(m)\). More... | |
| double | Mrun (const double mu_f, const double mu_i, const double m, const orders order=FULLNLO) const |
| Runs a quark mass from \(\mu_i\) to \(\mu_f\). More... | |
| double | Mrun4 (const double mu_f, const double mu_i, const double m) const |
| The running of a mass with the number of flavours \(n_f = 4\). More... | |
| double | MS2DRqmass (const double MSscale, const double MSbar) const |
| Converts a quark mass from the \(\overline{\mathrm{MS}}\) scheme to the \(\overline{\mathrm{DR}}\) scheme. More... | |
| double | MS2DRqmass (const double MSbar) const |
| Converts a quark mass from the \(\overline{\mathrm{MS}}\) scheme to the \(\overline{\mathrm{DR}}\) scheme. More... | |
| double | Nf (const double mu) const |
| The number of active flavour at scale \(\mu\). More... | |
| double | NfThresholdCorrections (double mu, double M, double als, int nf, orders order) const |
| Threshold corrections in matching als(nf+1) with als(nf) from eq. (34) of hep-ph/0512060. More... | |
| std::string | orderToString (const orders order) const |
| Converts an object of the enum type "orders" to the corresponding string. More... | |
| QCD () | |
| Constructor. More... | |
| void | setNc (double Nc) |
| A set method to change the number of colours \(N_c\). More... | |
| void | setOptionalParameter (std::string name, double value) |
| A method to set the parameter value for the parameters that are specific to only one set of observables. More... | |
| double | Thresholds (const int i) const |
| For accessing the active flavour threshold scales. More... | |
| Public Member Functions inherited from Model | |
| std::string | getModelName () const |
| A method to fetch the name of the model. More... | |
| const double & | getModelParam (std::string name) const |
| bool | isModelGeneralTHDM () const |
| bool | isModelGeorgiMachacek () const |
| bool | IsModelInitialized () const |
| A method to check if the model is initialized. More... | |
| bool | isModelLinearized () const |
| bool | isModelParam (std::string name) const |
| bool | isModelSUSY () const |
| bool | isModelTHDM () const |
| bool | isModelTHDMW () const |
| bool | IsUpdateError () const |
| A method to check if there was any error in the model update process. More... | |
| Model () | |
| The default constructor. More... | |
| void | setModelGeneralTHDM () |
| void | setModelGeorgiMachacek () |
| void | setModelInitialized (bool ModelInitialized) |
| A set method to fix the failure or success of the initialization of the model. More... | |
| void | setModelLinearized (bool linearized=true) |
| void | setModelName (const std::string name) |
| A method to set the name of the model. More... | |
| void | setModelSUSY () |
| void | setModelTHDM () |
| void | setModelTHDMW () |
| void | setSliced (bool Sliced) |
| void | setUpdateError (bool UpdateError) |
| A set method to fix the update status as success or failure. More... | |
| virtual | ~Model () |
| The default destructor. More... | |
Static Public Attributes | |
| static const int | NNPSMEFTd6Vars = 400 |
| The number of the model parameters in NPSMEFTd6. More... | |
| static const int | NNPSMEFTd6Vars_LFU_QFU = 204 |
| The number of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities. More... | |
| static const std::string | NPSMEFTd6Vars [NNPSMEFTd6Vars] |
| A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=false. More... | |
| static const std::string | NPSMEFTd6Vars_LFU_QFU [NNPSMEFTd6Vars_LFU_QFU] |
| A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=false. More... | |
| static const std::string | NPSMEFTd6VarsRot [NNPSMEFTd6Vars] |
| A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=true. More... | |
| static const std::string | NPSMEFTd6VarsRot_LFU_QFU [NNPSMEFTd6Vars_LFU_QFU] |
| A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=true. More... | |
| Static Public Attributes inherited from StandardModel | |
| static const double | GeVminus2_to_nb = 389379.338 |
| static const double | Mw_error = 0.00001 |
| The target accuracy of the iterative calculation of the \(W\)-boson mass in units of GeV. More... | |
| static const int | NSMvars = 26 |
| The number of the model parameters in StandardModel. More... | |
| static const int | NumSMParamsForEWPO = 33 |
| The number of the SM parameters that are relevant to the EW precision observables. More... | |
| static std::string | SMvars [NSMvars] |
| A string array containing the labels of the model parameters in StandardModel. More... | |
| Static Public Attributes inherited from QCD | |
| static const int | NQCDvars = 11 |
| The number of model parameters in QCD. More... | |
| static std::string | QCDvars [NQCDvars] |
| An array containing the labels under which all QCD parameters are stored in a vector of ModelParameter via InputParser::ReadParameters(). More... | |
Protected Member Functions | |
| gslpp::complex | CfB_diag (const Particle f) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{EB,UB,DB}\) corresponding to particle f. More... | |
| gslpp::complex | CfG_diag (const Particle f) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{UG,DG}\) corresponding to particle f. More... | |
| gslpp::complex | CfH_diag (const Particle f) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{EH,UH,DH}\) corresponding to particle f. More... | |
| gslpp::complex | CfW_diag (const Particle f) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{EW,UW,DW}\) corresponding to particle f. More... | |
| double | CHF1_diag (const Particle F) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(1)}\) corresponding to particle F. More... | |
| double | CHF3_diag (const Particle F) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(3)}\) corresponding to particle F. More... | |
| double | CHf_diag (const Particle f) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{HE,HU,HD}\) corresponding to particle f. More... | |
| gslpp::complex | CHud_diag (const Particle u) const |
| The diagonal entry of the dimension-6 operator coefficient \(C_{Hud}\) corresponding to particle f. More... | |
| virtual void | setParameter (const std::string name, const double &value) |
| A method to set the value of a parameter of the model. More... | |
| Protected Member Functions inherited from StandardModel | |
| double | AFB_NoISR_l (const QCD::lepton l_flavor, const double s) const |
| double | AFB_NoISR_q (const QCD::quark q_flavor, const double s) const |
| bool | checkEWPOscheme (const std::string scheme) const |
| A method to check if a given scheme name in string form is valid. More... | |
| virtual void | computeCKM () |
| The method to compute the CKM matrix. More... | |
| virtual void | computeYukawas () |
| The method to compute the Yukawa matrices. More... | |
| double | Delta_EWQCD (const QCD::quark q) const |
| The non-factorizable EW-QCD corrections to the partial widths for \(Z\to q\bar{q}\), denoted as \(\Delta_{\mathrm{EW/QCD}}\). More... | |
| double | getIntegrand_AFBnumeratorWithISR_bottom133 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom167 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom172 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom183 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom189 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom192 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom196 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom200 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom202 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom205 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_bottom207 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm133 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm167 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm172 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm183 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm189 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm192 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm196 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm200 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm202 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm205 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_charm207 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu130 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu136 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu161 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu172 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu183 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu189 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu192 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu196 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu200 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu202 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu205 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_mu207 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau130 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau136 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau161 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau172 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau183 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau189 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau192 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau196 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau200 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau202 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau205 (double x) const |
| double | getIntegrand_AFBnumeratorWithISR_tau207 (double x) const |
| double | getIntegrand_dsigmaBox_bottom130 (double x) const |
| double | getIntegrand_dsigmaBox_bottom133 (double x) const |
| double | getIntegrand_dsigmaBox_bottom136 (double x) const |
| double | getIntegrand_dsigmaBox_bottom161 (double x) const |
| double | getIntegrand_dsigmaBox_bottom167 (double x) const |
| double | getIntegrand_dsigmaBox_bottom172 (double x) const |
| double | getIntegrand_dsigmaBox_bottom183 (double x) const |
| double | getIntegrand_dsigmaBox_bottom189 (double x) const |
| double | getIntegrand_dsigmaBox_bottom192 (double x) const |
| double | getIntegrand_dsigmaBox_bottom196 (double x) const |
| double | getIntegrand_dsigmaBox_bottom200 (double x) const |
| double | getIntegrand_dsigmaBox_bottom202 (double x) const |
| double | getIntegrand_dsigmaBox_bottom205 (double x) const |
| double | getIntegrand_dsigmaBox_bottom207 (double x) const |
| double | getIntegrand_dsigmaBox_charm130 (double x) const |
| double | getIntegrand_dsigmaBox_charm133 (double x) const |
| double | getIntegrand_dsigmaBox_charm136 (double x) const |
| double | getIntegrand_dsigmaBox_charm161 (double x) const |
| double | getIntegrand_dsigmaBox_charm167 (double x) const |
| double | getIntegrand_dsigmaBox_charm172 (double x) const |
| double | getIntegrand_dsigmaBox_charm183 (double x) const |
| double | getIntegrand_dsigmaBox_charm189 (double x) const |
| double | getIntegrand_dsigmaBox_charm192 (double x) const |
| double | getIntegrand_dsigmaBox_charm196 (double x) const |
| double | getIntegrand_dsigmaBox_charm200 (double x) const |
| double | getIntegrand_dsigmaBox_charm202 (double x) const |
| double | getIntegrand_dsigmaBox_charm205 (double x) const |
| double | getIntegrand_dsigmaBox_charm207 (double x) const |
| double | getIntegrand_dsigmaBox_down130 (double x) const |
| double | getIntegrand_dsigmaBox_down133 (double x) const |
| double | getIntegrand_dsigmaBox_down136 (double x) const |
| double | getIntegrand_dsigmaBox_down161 (double x) const |
| double | getIntegrand_dsigmaBox_down167 (double x) const |
| double | getIntegrand_dsigmaBox_down172 (double x) const |
| double | getIntegrand_dsigmaBox_down183 (double x) const |
| double | getIntegrand_dsigmaBox_down189 (double x) const |
| double | getIntegrand_dsigmaBox_down192 (double x) const |
| double | getIntegrand_dsigmaBox_down196 (double x) const |
| double | getIntegrand_dsigmaBox_down200 (double x) const |
| double | getIntegrand_dsigmaBox_down202 (double x) const |
| double | getIntegrand_dsigmaBox_down205 (double x) const |
| double | getIntegrand_dsigmaBox_down207 (double x) const |
| double | getIntegrand_dsigmaBox_mu130 (double x) const |
| double | getIntegrand_dsigmaBox_mu133 (double x) const |
| double | getIntegrand_dsigmaBox_mu136 (double x) const |
| double | getIntegrand_dsigmaBox_mu161 (double x) const |
| double | getIntegrand_dsigmaBox_mu167 (double x) const |
| double | getIntegrand_dsigmaBox_mu172 (double x) const |
| double | getIntegrand_dsigmaBox_mu183 (double x) const |
| double | getIntegrand_dsigmaBox_mu189 (double x) const |
| double | getIntegrand_dsigmaBox_mu192 (double x) const |
| double | getIntegrand_dsigmaBox_mu196 (double x) const |
| double | getIntegrand_dsigmaBox_mu200 (double x) const |
| double | getIntegrand_dsigmaBox_mu202 (double x) const |
| double | getIntegrand_dsigmaBox_mu205 (double x) const |
| double | getIntegrand_dsigmaBox_mu207 (double x) const |
| double | getIntegrand_dsigmaBox_strange130 (double x) const |
| double | getIntegrand_dsigmaBox_strange133 (double x) const |
| double | getIntegrand_dsigmaBox_strange136 (double x) const |
| double | getIntegrand_dsigmaBox_strange161 (double x) const |
| double | getIntegrand_dsigmaBox_strange167 (double x) const |
| double | getIntegrand_dsigmaBox_strange172 (double x) const |
| double | getIntegrand_dsigmaBox_strange183 (double x) const |
| double | getIntegrand_dsigmaBox_strange189 (double x) const |
| double | getIntegrand_dsigmaBox_strange192 (double x) const |
| double | getIntegrand_dsigmaBox_strange196 (double x) const |
| double | getIntegrand_dsigmaBox_strange200 (double x) const |
| double | getIntegrand_dsigmaBox_strange202 (double x) const |
| double | getIntegrand_dsigmaBox_strange205 (double x) const |
| double | getIntegrand_dsigmaBox_strange207 (double x) const |
| double | getIntegrand_dsigmaBox_tau130 (double x) const |
| double | getIntegrand_dsigmaBox_tau133 (double x) const |
| double | getIntegrand_dsigmaBox_tau136 (double x) const |
| double | getIntegrand_dsigmaBox_tau161 (double x) const |
| double | getIntegrand_dsigmaBox_tau167 (double x) const |
| double | getIntegrand_dsigmaBox_tau172 (double x) const |
| double | getIntegrand_dsigmaBox_tau183 (double x) const |
| double | getIntegrand_dsigmaBox_tau189 (double x) const |
| double | getIntegrand_dsigmaBox_tau192 (double x) const |
| double | getIntegrand_dsigmaBox_tau196 (double x) const |
| double | getIntegrand_dsigmaBox_tau200 (double x) const |
| double | getIntegrand_dsigmaBox_tau202 (double x) const |
| double | getIntegrand_dsigmaBox_tau205 (double x) const |
| double | getIntegrand_dsigmaBox_tau207 (double x) const |
| double | getIntegrand_dsigmaBox_up130 (double x) const |
| double | getIntegrand_dsigmaBox_up133 (double x) const |
| double | getIntegrand_dsigmaBox_up136 (double x) const |
| double | getIntegrand_dsigmaBox_up161 (double x) const |
| double | getIntegrand_dsigmaBox_up167 (double x) const |
| double | getIntegrand_dsigmaBox_up172 (double x) const |
| double | getIntegrand_dsigmaBox_up183 (double x) const |
| double | getIntegrand_dsigmaBox_up189 (double x) const |
| double | getIntegrand_dsigmaBox_up192 (double x) const |
| double | getIntegrand_dsigmaBox_up196 (double x) const |
| double | getIntegrand_dsigmaBox_up200 (double x) const |
| double | getIntegrand_dsigmaBox_up202 (double x) const |
| double | getIntegrand_dsigmaBox_up205 (double x) const |
| double | getIntegrand_dsigmaBox_up207 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom130 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom133 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom136 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom161 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom167 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom172 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom183 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom189 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom192 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom196 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom200 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom202 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom205 (double x) const |
| double | getIntegrand_sigmaWithISR_bottom207 (double x) const |
| double | getIntegrand_sigmaWithISR_charm130 (double x) const |
| double | getIntegrand_sigmaWithISR_charm133 (double x) const |
| double | getIntegrand_sigmaWithISR_charm136 (double x) const |
| double | getIntegrand_sigmaWithISR_charm161 (double x) const |
| double | getIntegrand_sigmaWithISR_charm167 (double x) const |
| double | getIntegrand_sigmaWithISR_charm172 (double x) const |
| double | getIntegrand_sigmaWithISR_charm183 (double x) const |
| double | getIntegrand_sigmaWithISR_charm189 (double x) const |
| double | getIntegrand_sigmaWithISR_charm192 (double x) const |
| double | getIntegrand_sigmaWithISR_charm196 (double x) const |
| double | getIntegrand_sigmaWithISR_charm200 (double x) const |
| double | getIntegrand_sigmaWithISR_charm202 (double x) const |
| double | getIntegrand_sigmaWithISR_charm205 (double x) const |
| double | getIntegrand_sigmaWithISR_charm207 (double x) const |
| double | getIntegrand_sigmaWithISR_down130 (double x) const |
| double | getIntegrand_sigmaWithISR_down133 (double x) const |
| double | getIntegrand_sigmaWithISR_down136 (double x) const |
| double | getIntegrand_sigmaWithISR_down161 (double x) const |
| double | getIntegrand_sigmaWithISR_down167 (double x) const |
| double | getIntegrand_sigmaWithISR_down172 (double x) const |
| double | getIntegrand_sigmaWithISR_down183 (double x) const |
| double | getIntegrand_sigmaWithISR_down189 (double x) const |
| double | getIntegrand_sigmaWithISR_down192 (double x) const |
| double | getIntegrand_sigmaWithISR_down196 (double x) const |
| double | getIntegrand_sigmaWithISR_down200 (double x) const |
| double | getIntegrand_sigmaWithISR_down202 (double x) const |
| double | getIntegrand_sigmaWithISR_down205 (double x) const |
| double | getIntegrand_sigmaWithISR_down207 (double x) const |
| double | getIntegrand_sigmaWithISR_mu130 (double x) const |
| double | getIntegrand_sigmaWithISR_mu136 (double x) const |
| double | getIntegrand_sigmaWithISR_mu161 (double x) const |
| double | getIntegrand_sigmaWithISR_mu172 (double x) const |
| double | getIntegrand_sigmaWithISR_mu183 (double x) const |
| double | getIntegrand_sigmaWithISR_mu189 (double x) const |
| double | getIntegrand_sigmaWithISR_mu192 (double x) const |
| double | getIntegrand_sigmaWithISR_mu196 (double x) const |
| double | getIntegrand_sigmaWithISR_mu200 (double x) const |
| double | getIntegrand_sigmaWithISR_mu202 (double x) const |
| double | getIntegrand_sigmaWithISR_mu205 (double x) const |
| double | getIntegrand_sigmaWithISR_mu207 (double x) const |
| double | getIntegrand_sigmaWithISR_strange130 (double x) const |
| double | getIntegrand_sigmaWithISR_strange133 (double x) const |
| double | getIntegrand_sigmaWithISR_strange136 (double x) const |
| double | getIntegrand_sigmaWithISR_strange161 (double x) const |
| double | getIntegrand_sigmaWithISR_strange167 (double x) const |
| double | getIntegrand_sigmaWithISR_strange172 (double x) const |
| double | getIntegrand_sigmaWithISR_strange183 (double x) const |
| double | getIntegrand_sigmaWithISR_strange189 (double x) const |
| double | getIntegrand_sigmaWithISR_strange192 (double x) const |
| double | getIntegrand_sigmaWithISR_strange196 (double x) const |
| double | getIntegrand_sigmaWithISR_strange200 (double x) const |
| double | getIntegrand_sigmaWithISR_strange202 (double x) const |
| double | getIntegrand_sigmaWithISR_strange205 (double x) const |
| double | getIntegrand_sigmaWithISR_strange207 (double x) const |
| double | getIntegrand_sigmaWithISR_tau130 (double x) const |
| double | getIntegrand_sigmaWithISR_tau136 (double x) const |
| double | getIntegrand_sigmaWithISR_tau161 (double x) const |
| double | getIntegrand_sigmaWithISR_tau172 (double x) const |
| double | getIntegrand_sigmaWithISR_tau183 (double x) const |
| double | getIntegrand_sigmaWithISR_tau189 (double x) const |
| double | getIntegrand_sigmaWithISR_tau192 (double x) const |
| double | getIntegrand_sigmaWithISR_tau196 (double x) const |
| double | getIntegrand_sigmaWithISR_tau200 (double x) const |
| double | getIntegrand_sigmaWithISR_tau202 (double x) const |
| double | getIntegrand_sigmaWithISR_tau205 (double x) const |
| double | getIntegrand_sigmaWithISR_tau207 (double x) const |
| double | getIntegrand_sigmaWithISR_up130 (double x) const |
| double | getIntegrand_sigmaWithISR_up133 (double x) const |
| double | getIntegrand_sigmaWithISR_up136 (double x) const |
| double | getIntegrand_sigmaWithISR_up161 (double x) const |
| double | getIntegrand_sigmaWithISR_up167 (double x) const |
| double | getIntegrand_sigmaWithISR_up172 (double x) const |
| double | getIntegrand_sigmaWithISR_up183 (double x) const |
| double | getIntegrand_sigmaWithISR_up189 (double x) const |
| double | getIntegrand_sigmaWithISR_up192 (double x) const |
| double | getIntegrand_sigmaWithISR_up196 (double x) const |
| double | getIntegrand_sigmaWithISR_up200 (double x) const |
| double | getIntegrand_sigmaWithISR_up202 (double x) const |
| double | getIntegrand_sigmaWithISR_up205 (double x) const |
| double | getIntegrand_sigmaWithISR_up207 (double x) const |
| double | Integrand_AFBnumeratorWithISR_l (double x, const QCD::lepton l_flavor, const double s) const |
| double | Integrand_AFBnumeratorWithISR_q (double x, const QCD::quark q_flavor, const double s) const |
| double | Integrand_dsigmaBox_l (double cosTheta, const QCD::lepton l_flavor, const double s) const |
| double | Integrand_dsigmaBox_q (double cosTheta, const QCD::quark q_flavor, const double s) const |
| double | Integrand_sigmaWithISR_l (double x, const QCD::lepton l_flavor, const double s) const |
| double | Integrand_sigmaWithISR_q (double x, const QCD::quark q_flavor, const double s) const |
| double | m_q (const QCD::quark q, const double mu, const orders order=FULLNLO) const |
| double | RAq (const QCD::quark q) const |
| The radiator factor associated with the final-state QED and QCD corrections to the the axial-vector-current interactions, \(R_A^q(M_Z^2)\). More... | |
| double | resumKappaZ (const double DeltaRho[orders_EW_size], const double deltaKappa_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const |
| A method to compute the real part of the effetvive coupling \(\kappa_Z^f\) from \(\Delta\rho\), \(\delta\rho_{\rm rem}^{f}\) and \(\Delta r_{\mathrm{rem}}\). More... | |
| double | resumMw (const double Mw_i, const double DeltaRho[orders_EW_size], const double DeltaR_rem[orders_EW_size]) const |
| A method to compute the \(W\)-boson mass from \(\Delta\rho\) and \(\Delta r_{\mathrm{rem}}\). More... | |
| double | resumRhoZ (const double DeltaRho[orders_EW_size], const double deltaRho_rem[orders_EW_size], const double DeltaRbar_rem, const bool bool_Zbb) const |
| A method to compute the real part of the effective coupling \(\rho_Z^f\) from \(\Delta\rho\), \(\delta\rho_{\rm rem}^{f}\) and \(\Delta r_{\mathrm{rem}}\). More... | |
| double | RVh () const |
| The singlet vector corrections to the hadronic \(Z\)-boson width, denoted as \(R_V^h\). More... | |
| double | RVq (const QCD::quark q) const |
| The radiator factor associated with the final-state QED and QCD corrections to the the vector-current interactions, \(R_V^q(M_Z^2)\). More... | |
| double | SchemeToDouble (const std::string scheme) const |
| A method to convert a given scheme name in string form into a floating-point number with double precision. More... | |
| double | sigma_NoISR_l (const QCD::lepton l_flavor, const double s) const |
| double | sigma_NoISR_q (const QCD::quark q_flavor, const double s) const |
| double | taub () const |
| Top-mass corrections to the \(Zb\bar{b}\) vertex, denoted by \(\tau_b\). More... | |
| Protected Member Functions inherited from QCD | |
| double | MassOfNf (int nf) const |
| The Mbar mass of the heaviest quark in the theory with Nf active flavour. More... | |
Protected Attributes | |
| double | aleMz |
| The em constant at Mz. More... | |
| double | BrHexo |
| The branching ratio of exotic (not invisible) Higgs decays. More... | |
| double | BrHinv |
| The branching ratio of invisible Higgs decays. More... | |
| double | C2B |
| The dimension-6 operator coefficient \(C_{2W}\). More... | |
| double | C2W |
| The dimension-6 operator coefficient \(C_{2B}\). More... | |
| double | CdH_11i |
| The dimension-6 operator coefficient \((C_{dH})_{11}\) (imaginary part). More... | |
| double | CdH_11r |
| The dimension-6 operator coefficient \((C_{dH})_{11}\) (real part). More... | |
| double | CdH_12i |
| The dimension-6 operator coefficient \((C_{dH})_{12}\) (imaginary part). More... | |
| double | CdH_12r |
| The dimension-6 operator coefficient \((C_{dH})_{12}\) (real part). More... | |
| double | CdH_13i |
| The dimension-6 operator coefficient \((C_{dH})_{13}\) (imaginary part). More... | |
| double | CdH_13r |
| The dimension-6 operator coefficient \((C_{dH})_{13}\) (real part). More... | |
| double | CdH_22i |
| The dimension-6 operator coefficient \((C_{dH})_{22}\) (imaginary part). More... | |
| double | CdH_22r |
| The dimension-6 operator coefficient \((C_{dH})_{22}\) (real part). More... | |
| double | CdH_23i |
| The dimension-6 operator coefficient \((C_{dH})_{23}\) (imaginary part). More... | |
| double | CdH_23r |
| The dimension-6 operator coefficient \((C_{dH})_{23}\) (real part). More... | |
| double | CdH_33i |
| The dimension-6 operator coefficient \((C_{dH})_{33}\) (imaginary part). More... | |
| double | CdH_33r |
| The dimension-6 operator coefficient \((C_{dH})_{33}\) (real part). More... | |
| double | CDHB |
| The dimension-6 operator coefficient \(C_{DHB}\). More... | |
| double | CDHW |
| The dimension-6 operator coefficient \(C_{DHW}\). More... | |
| double | Ced_1111 |
| double | Ced_1122 |
| double | Ced_1123 |
| double | Ced_1132 |
| double | Ced_1133 |
| double | Ced_2211 |
| double | Ced_2223 |
| double | Ced_2232 |
| double | Ced_3311 |
| double | Ced_3323 |
| double | Ced_3332 |
| double | Cee_1111 |
| double | Cee_1122 |
| double | Cee_1133 |
| double | Cee_2211 |
| double | Cee_3311 |
| double | CeH_11i |
| The dimension-6 operator coefficient \((C_{eH})_{11}\) (imaginary part). More... | |
| double | CeH_11r |
| The dimension-6 operator coefficient \((C_{eH})_{11}\) (real part). More... | |
| double | CeH_12i |
| The dimension-6 operator coefficient \((C_{eH})_{12}\) (imaginary part). More... | |
| double | CeH_12r |
| The dimension-6 operator coefficient \((C_{eH})_{12}\) (real part). More... | |
| double | CeH_13i |
| The dimension-6 operator coefficient \((C_{eH})_{13}\) (imaginary part). More... | |
| double | CeH_13r |
| The dimension-6 operator coefficient \((C_{eH})_{13}\) (real part). More... | |
| double | CeH_22i |
| The dimension-6 operator coefficient \((C_{eH})_{22}\) (imaginary part). More... | |
| double | CeH_22r |
| The dimension-6 operator coefficient \((C_{eH})_{22}\) (real part). More... | |
| double | CeH_23i |
| The dimension-6 operator coefficient \((C_{eH})_{23}\) (imaginary part). More... | |
| double | CeH_23r |
| The dimension-6 operator coefficient \((C_{eH})_{23}\) (real part). More... | |
| double | CeH_33i |
| The dimension-6 operator coefficient \((C_{eH})_{33}\) (imaginary part). More... | |
| double | CeH_33r |
| The dimension-6 operator coefficient \((C_{eH})_{33}\) (real part). More... | |
| double | Ceu_1111 |
| double | Ceu_1122 |
| double | Ceu_1133 |
| double | Ceu_2211 |
| double | Ceu_2233 |
| double | Ceu_3311 |
| double | CG |
| The dimension-6 operator coefficient \(C_{G}\). More... | |
| double | CH |
| The dimension-6 operator coefficient \(C_{H}\). More... | |
| double | CHB |
| The dimension-6 operator coefficient \(C_{HB}\). More... | |
| double | CHbox |
| The dimension-6 operator coefficient \(C_{H\Box}\). More... | |
| double | CHD |
| The dimension-6 operator coefficient \(C_{HD}\). More... | |
| double | CHd_11 |
| The dimension-6 operator coefficient \((C_{Hd})_{11}\). More... | |
| double | CHd_12i |
| The dimension-6 operator coefficient \((C_{Hd})_{12}\) (imaginary part). More... | |
| double | CHd_12r |
| The dimension-6 operator coefficient \((C_{Hd})_{12}\) (real part). More... | |
| double | CHd_13i |
| The dimension-6 operator coefficient \((C_{Hd})_{13}\) (imaginary part). More... | |
| double | CHd_13r |
| The dimension-6 operator coefficient \((C_{Hd})_{13}\) (real part). More... | |
| double | CHd_22 |
| The dimension-6 operator coefficient \((C_{Hd})_{22}\). More... | |
| double | CHd_23i |
| The dimension-6 operator coefficient \((C_{Hd})_{23}\) (imaginary part). More... | |
| double | CHd_23r |
| The dimension-6 operator coefficient \((C_{Hd})_{23}\) (real part). More... | |
| double | CHd_33 |
| The dimension-6 operator coefficient \((C_{Hd})_{33}\). More... | |
| double | CHe_11 |
| The dimension-6 operator coefficient \((C_{He})_{11}\). More... | |
| double | CHe_12i |
| The dimension-6 operator coefficient \((C_{He})_{12}\) (imaginary part). More... | |
| double | CHe_12r |
| The dimension-6 operator coefficient \((C_{He})_{12}\) (real part). More... | |
| double | CHe_13i |
| The dimension-6 operator coefficient \((C_{He})_{13}\) (imaginary part). More... | |
| double | CHe_13r |
| The dimension-6 operator coefficient \((C_{He})_{13}\) (real part). More... | |
| double | CHe_22 |
| The dimension-6 operator coefficient \((C_{He})_{22}\). More... | |
| double | CHe_23i |
| The dimension-6 operator coefficient \((C_{He})_{23}\) (imaginary part). More... | |
| double | CHe_23r |
| The dimension-6 operator coefficient \((C_{He})_{23}\) (real part). More... | |
| double | CHe_33 |
| The dimension-6 operator coefficient \((C_{He})_{33}\). More... | |
| double | CHG |
| The dimension-6 operator coefficient \(C_{HG}\). More... | |
| double | CHL1_11 |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{11}\). More... | |
| double | CHL1_12i |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (imaginary part). More... | |
| double | CHL1_12r |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (real part). More... | |
| double | CHL1_13i |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (imaginary part). More... | |
| double | CHL1_13r |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (real part). More... | |
| double | CHL1_22 |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{22}\). More... | |
| double | CHL1_23i |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (imaginary part). More... | |
| double | CHL1_23r |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (real part). More... | |
| double | CHL1_33 |
| The dimension-6 operator coefficient \((C_{HL}^{(1)})_{33}\). More... | |
| double | CHL3_11 |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{11}\). More... | |
| double | CHL3_12i |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part). More... | |
| double | CHL3_12r |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part). More... | |
| double | CHL3_13i |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part). More... | |
| double | CHL3_13r |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part). More... | |
| double | CHL3_22 |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{22}\). More... | |
| double | CHL3_23i |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part). More... | |
| double | CHL3_23r |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part). More... | |
| double | CHL3_33 |
| The dimension-6 operator coefficient \((C_{HL}^{(3)})_{33}\). More... | |
| double | CHQ1_11 |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{11}\). More... | |
| double | CHQ1_12i |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (imaginary part). More... | |
| double | CHQ1_12r |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (real part). More... | |
| double | CHQ1_13i |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (imaginary part). More... | |
| double | CHQ1_13r |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (real part). More... | |
| double | CHQ1_22 |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{22}\). More... | |
| double | CHQ1_23i |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (imaginary part). More... | |
| double | CHQ1_23r |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (real part). More... | |
| double | CHQ1_33 |
| The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{33}\). More... | |
| double | CHQ3_11 |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{11}\). More... | |
| double | CHQ3_12i |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (imaginary part). More... | |
| double | CHQ3_12r |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (real part). More... | |
| double | CHQ3_13i |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (imaginary part). More... | |
| double | CHQ3_13r |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (real part). More... | |
| double | CHQ3_22 |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{22}\). More... | |
| double | CHQ3_23i |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (imaginary part). More... | |
| double | CHQ3_23r |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (real part). More... | |
| double | CHQ3_33 |
| The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{33}\). More... | |
| double | cHSM |
| Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes. More... | |
| double | CHu_11 |
| The dimension-6 operator coefficient \((C_{Hu})_{11}\). More... | |
| double | CHu_12i |
| The dimension-6 operator coefficient \((C_{Hu})_{12}\) (imaginary part). More... | |
| double | CHu_12r |
| The dimension-6 operator coefficient \((C_{Hu})_{12}\) (real part). More... | |
| double | CHu_13i |
| The dimension-6 operator coefficient \((C_{Hu})_{13}\) (imaginary part). More... | |
| double | CHu_13r |
| The dimension-6 operator coefficient \((C_{Hu})_{13}\) (real part). More... | |
| double | CHu_22 |
| The dimension-6 operator coefficient \((C_{Hu})_{22}\). More... | |
| double | CHu_23i |
| The dimension-6 operator coefficient \((C_{Hu})_{23}\) (imaginary part). More... | |
| double | CHu_23r |
| The dimension-6 operator coefficient \((C_{Hu})_{23}\) (real part). More... | |
| double | CHu_33 |
| The dimension-6 operator coefficient \((C_{Hu})_{33}\). More... | |
| double | CHud_11i |
| The dimension-6 operator coefficient \((C_{Hud})_{11}\) (imaginary part). More... | |
| double | CHud_11r |
| The dimension-6 operator coefficient \((C_{Hud})_{11}\) (real part). More... | |
| double | CHud_12i |
| The dimension-6 operator coefficient \((C_{Hud})_{12}\) (imaginary part). More... | |
| double | CHud_12r |
| The dimension-6 operator coefficient \((C_{Hud})_{12}\) (real part). More... | |
| double | CHud_13i |
| The dimension-6 operator coefficient \((C_{Hud})_{13}\) (imaginary part). More... | |
| double | CHud_13r |
| The dimension-6 operator coefficient \((C_{Hud})_{13}\) (real part). More... | |
| double | CHud_22i |
| The dimension-6 operator coefficient \((C_{Hud})_{22}\) (imaginary part). More... | |
| double | CHud_22r |
| The dimension-6 operator coefficient \((C_{Hud})_{22}\) (real part). More... | |
| double | CHud_23i |
| The dimension-6 operator coefficient \((C_{Hud})_{23}\) (imaginary part). More... | |
| double | CHud_23r |
| The dimension-6 operator coefficient \((C_{Hud})_{23}\) (real part). More... | |
| double | CHud_33i |
| The dimension-6 operator coefficient \((C_{Hud})_{33}\) (imaginary part). More... | |
| double | CHud_33r |
| The dimension-6 operator coefficient \((C_{Hud})_{33}\) (real part). More... | |
| double | CHW |
| The dimension-6 operator coefficient \(C_{HW}\). More... | |
| double | CHWB |
| The dimension-6 operator coefficient \(C_{HWB}\). More... | |
| double | CHWHB_gaga |
| The combination of dimension-6 operator coefficients entering in \(\delta_{AA}\): \(s_W^2 C_{HW} + c_W^2 C_{HW}\). More... | |
| double | CHWHB_gagaorth |
| The combination of dimension-6 operator coefficients \(-c_W^2 C_{HW} + s_W^2 C_{HW}\). More... | |
| double | CLd_1111 |
| double | CLd_1122 |
| double | CLd_1123 |
| double | CLd_1132 |
| double | CLd_1133 |
| double | CLd_2211 |
| double | CLd_2223 |
| double | CLd_2232 |
| double | CLd_3311 |
| double | CLd_3323 |
| double | CLd_3332 |
| double | CLe_1111 |
| double | CLe_1122 |
| double | CLe_1133 |
| double | CLe_2211 |
| double | CLe_3311 |
| double | CLedQ_11 |
| double | CLedQ_22 |
| double | cLH3d62 |
| Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions modifying the Higgs trilinear coupling (Quadratic terms). More... | |
| double | cLHd6 |
| Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions. More... | |
| double | CLL_1111 |
| double | CLL_1122 |
| double | CLL_1133 |
| double | CLL_1221 |
| double | CLL_1331 |
| double | CLL_2112 |
| double | CLL_2211 |
| double | CLL_3113 |
| double | CLL_3311 |
| double | CLQ1_1111 |
| double | CLQ1_1122 |
| double | CLQ1_1123 |
| double | CLQ1_1132 |
| double | CLQ1_1133 |
| double | CLQ1_1221 |
| double | CLQ1_1331 |
| double | CLQ1_2112 |
| double | CLQ1_2211 |
| double | CLQ1_2223 |
| double | CLQ1_2232 |
| double | CLQ1_3113 |
| double | CLQ1_3311 |
| double | CLQ1_3323 |
| double | CLQ1_3332 |
| double | CLQ3_1111 |
| double | CLQ3_1122 |
| double | CLQ3_1123 |
| double | CLQ3_1132 |
| double | CLQ3_1133 |
| double | CLQ3_1221 |
| double | CLQ3_1331 |
| double | CLQ3_2112 |
| double | CLQ3_2211 |
| double | CLQ3_2223 |
| double | CLQ3_2232 |
| double | CLQ3_3113 |
| double | CLQ3_3311 |
| double | CLQ3_3323 |
| double | CLQ3_3332 |
| double | CLu_1111 |
| double | CLu_1122 |
| double | CLu_1133 |
| double | CLu_2211 |
| double | CLu_2233 |
| double | CLu_3311 |
| double | CpLedQ_11 |
| double | CpLedQ_22 |
| double | CQe_1111 |
| double | CQe_1122 |
| double | CQe_1133 |
| double | CQe_2211 |
| double | CQe_2311 |
| double | CQe_2322 |
| double | CQe_2333 |
| double | CQe_3211 |
| double | CQe_3222 |
| double | CQe_3233 |
| double | CQe_3311 |
| double | CuB_11i |
| The dimension-6 operator coefficient \((C_{uB})_{11}\) (imaginary part). More... | |
| double | CuB_11r |
| The dimension-6 operator coefficient \((C_{uB})_{11}\) (real part). More... | |
| double | CuB_12i |
| The dimension-6 operator coefficient \((C_{uB})_{12}\) (imaginary part). More... | |
| double | CuB_12r |
| The dimension-6 operator coefficient \((C_{uB})_{12}\) (real part). More... | |
| double | CuB_13i |
| The dimension-6 operator coefficient \((C_{uB})_{13}\) (imaginary part). More... | |
| double | CuB_13r |
| The dimension-6 operator coefficient \((C_{uB})_{13}\) (real part). More... | |
| double | CuB_22i |
| The dimension-6 operator coefficient \((C_{uB})_{22}\) (imaginary part). More... | |
| double | CuB_22r |
| The dimension-6 operator coefficient \((C_{uB})_{22}\) (real part). More... | |
| double | CuB_23i |
| The dimension-6 operator coefficient \((C_{uB})_{23}\) (imaginary part). More... | |
| double | CuB_23r |
| The dimension-6 operator coefficient \((C_{uB})_{23}\) (real part). More... | |
| double | CuB_33i |
| The dimension-6 operator coefficient \((C_{uB})_{33}\) (imaginary part). More... | |
| double | CuB_33r |
| The dimension-6 operator coefficient \((C_{uB})_{33}\) (real part). More... | |
| double | CuG_11i |
| The dimension-6 operator coefficient \((C_{uG})_{11}\) (imaginary part). More... | |
| double | CuG_11r |
| The dimension-6 operator coefficient \((C_{uG})_{11}\) (real part). More... | |
| double | CuG_12i |
| The dimension-6 operator coefficient \((C_{uG})_{12}\) (imaginary part). More... | |
| double | CuG_12r |
| The dimension-6 operator coefficient \((C_{uG})_{12}\) (real part). More... | |
| double | CuG_13i |
| The dimension-6 operator coefficient \((C_{uG})_{13}\) (imaginary part). More... | |
| double | CuG_13r |
| The dimension-6 operator coefficient \((C_{uG})_{13}\) (real part). More... | |
| double | CuG_22i |
| The dimension-6 operator coefficient \((C_{uG})_{22}\) (imaginary part). More... | |
| double | CuG_22r |
| The dimension-6 operator coefficient \((C_{uG})_{22}\) (real part). More... | |
| double | CuG_23i |
| The dimension-6 operator coefficient \((C_{uG})_{23}\) (imaginary part). More... | |
| double | CuG_23r |
| The dimension-6 operator coefficient \((C_{uG})_{23}\) (real part). More... | |
| double | CuG_33i |
| The dimension-6 operator coefficient \((C_{uG})_{33}\) (imaginary part). More... | |
| double | CuG_33r |
| The dimension-6 operator coefficient \((C_{uG})_{33}\) (real part). More... | |
| double | CuH_11i |
| The dimension-6 operator coefficient \((C_{uH})_{11}\) (imaginary part). More... | |
| double | CuH_11r |
| The dimension-6 operator coefficient \((C_{uH})_{11}\) (real part). More... | |
| double | CuH_12i |
| The dimension-6 operator coefficient \((C_{uH})_{12}\) (imaginary part). More... | |
| double | CuH_12r |
| The dimension-6 operator coefficient \((C_{uH})_{12}\) (real part). More... | |
| double | CuH_13i |
| The dimension-6 operator coefficient \((C_{uH})_{13}\) (imaginary part). More... | |
| double | CuH_13r |
| The dimension-6 operator coefficient \((C_{uH})_{13}\) (real part). More... | |
| double | CuH_22i |
| The dimension-6 operator coefficient \((C_{uH})_{22}\) (imaginary part). More... | |
| double | CuH_22r |
| The dimension-6 operator coefficient \((C_{uH})_{22}\) (real part). More... | |
| double | CuH_23i |
| The dimension-6 operator coefficient \((C_{uH})_{23}\) (imaginary part). More... | |
| double | CuH_23r |
| The dimension-6 operator coefficient \((C_{uH})_{23}\) (real part). More... | |
| double | CuH_33i |
| The dimension-6 operator coefficient \((C_{uH})_{33}\) (imaginary part). More... | |
| double | CuH_33r |
| The dimension-6 operator coefficient \((C_{uH})_{33}\) (real part). More... | |
| double | CuW_11i |
| The dimension-6 operator coefficient \((C_{uW})_{11}\) (imaginary part). More... | |
| double | CuW_11r |
| The dimension-6 operator coefficient \((C_{uW})_{11}\) (real part). More... | |
| double | CuW_12i |
| The dimension-6 operator coefficient \((C_{uW})_{12}\) (imaginary part). More... | |
| double | CuW_12r |
| The dimension-6 operator coefficient \((C_{uW})_{12}\) (real part). More... | |
| double | CuW_13i |
| The dimension-6 operator coefficient \((C_{uW})_{13}\) (imaginary part). More... | |
| double | CuW_13r |
| The dimension-6 operator coefficient \((C_{uW})_{13}\) (real part). More... | |
| double | CuW_22i |
| The dimension-6 operator coefficient \((C_{uW})_{22}\) (imaginary part). More... | |
| double | CuW_22r |
| The dimension-6 operator coefficient \((C_{uW})_{22}\) (real part). More... | |
| double | CuW_23i |
| The dimension-6 operator coefficient \((C_{uW})_{23}\) (imaginary part). More... | |
| double | CuW_23r |
| The dimension-6 operator coefficient \((C_{uW})_{23}\) (real part). More... | |
| double | CuW_33i |
| The dimension-6 operator coefficient \((C_{uW})_{33}\) (imaginary part). More... | |
| double | CuW_33r |
| The dimension-6 operator coefficient \((C_{uW})_{33}\) (real part). More... | |
| double | CW |
| The dimension-6 operator coefficient \(C_{W}\). More... | |
| double | cW2_tree |
| The square of the tree level values for the cosine of the weak angle. More... | |
| double | cW_tree |
| The tree level values for the cosine of the weak angle. More... | |
| double | delta_AA |
| Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition. More... | |
| double | delta_AZ |
| Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition. More... | |
| double | delta_h |
| Combinations of dimension 6 coefficients modifying the \(H\) canonical field definition. More... | |
| double | delta_ZZ |
| Combination of dimension 6 coefficients modifying the \(Z_\mu\) canonical field definition. More... | |
| double | dg1Z |
| Independent contribution to aTGC. More... | |
| double | dGammaHTotR1 |
| double | dGammaHTotR2 |
| double | dKappaga |
| Independent contribution to aTGC. More... | |
| double | dZH |
| Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization. More... | |
| double | eeettHint |
| Intrinsic relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.) More... | |
| double | eeettHpar |
| Parametric relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.) More... | |
| double | eeeWBFint |
| Intrinsic relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.) More... | |
| double | eeeWBFpar |
| Parametric relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.) More... | |
| double | eeeZHint |
| Intrinsic relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.) More... | |
| double | eeeZHpar |
| Parametric relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.) More... | |
| double | eeMz |
| The em coupling at Mz. More... | |
| double | eeMz2 |
| The em coupling squared (at Mz). More... | |
| double | eggFint |
| Intrinsic relative theoretical error in ggF production. (Assumed to be constant in energy.) More... | |
| double | eggFpar |
| Parametric relative theoretical error in ggF production. (Assumed to be constant in energy.) More... | |
| double | eHbbint |
| Intrinsic relative theoretical error in \(H \to b\bar{b}\). More... | |
| double | eHbbpar |
| Parametric relative theoretical error in \(H \to b\bar{b}\). More... | |
| double | eHccint |
| Intrinsic relative theoretical error in \(H \to c\bar{c}\). More... | |
| double | eHccpar |
| Parametric relative theoretical error in \(H \to c\bar{c}\). More... | |
| double | eHgagaint |
| Intrinsic relative theoretical error in \(H \to \gamma\gamma\). More... | |
| double | eHgagapar |
| Parametric relative theoretical error in \(H \to \gamma\gamma\). More... | |
| double | eHggint |
| Intrinsic relative theoretical error in \(H \to g g\). More... | |
| double | eHggpar |
| Parametric relative theoretical error in \(H \to g g\). More... | |
| double | eHmumuint |
| Intrinsic relative theoretical error in \(H \to \mu^+ \mu^-\). More... | |
| double | eHmumupar |
| Parametric relative theoretical error in \(H \to \mu^+ \mu^-\). More... | |
| double | eHtautauint |
| Intrinsic relative theoretical error in \(H \to \tau^+ \tau^-\). More... | |
| double | eHtautaupar |
| Parametric relative theoretical error in \(H \to \tau^+ \tau^-\). More... | |
| double | eHWWint |
| Intrinsic relative theoretical error in \(H \to W W\). More... | |
| double | eHWWpar |
| Parametric relative theoretical error in \(H \to W W\). More... | |
| double | eHZgaint |
| Intrinsic relative theoretical error in \(H \to Z \gamma\). More... | |
| double | eHZgapar |
| Parametric relative theoretical error in \(H \to Z \gamma\). More... | |
| double | eHZZint |
| Intrinsic relative theoretical error in \(H \to Z Z\). More... | |
| double | eHZZpar |
| Parametric relative theoretical error in \(H \to Z Z\). More... | |
| double | ettH_1314_DeltagHt |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (13 & 14 TeV). More... | |
| double | ettH_1314_G |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (13 & 14 TeV). More... | |
| double | ettH_1314_HG |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (13 & 14 TeV). More... | |
| double | ettH_1314_uG_33r |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (13 & 14 TeV). More... | |
| double | ettH_2_DeltagHt |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (1.96 TeV). More... | |
| double | ettH_2_G |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (1.96 TeV). More... | |
| double | ettH_2_HG |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (1.96 TeV). More... | |
| double | ettH_2_uG_33r |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (1.96 TeV). More... | |
| double | ettH_78_DeltagHt |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (7 & 8 TeV). More... | |
| double | ettH_78_G |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (7 & 8 TeV). More... | |
| double | ettH_78_HG |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (7 & 8 TeV). More... | |
| double | ettH_78_uG_33r |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (7 & 8 TeV). More... | |
| double | ettHint |
| Intrinsic relative theoretical error in ttH production. (Assumed to be constant in energy.) More... | |
| double | ettHpar |
| Parametric relative theoretical error in ttH production. (Assumed to be constant in energy.) More... | |
| double | eVBF_1314_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_DHB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_HB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_Hd_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_HG |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_HQ1_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_Hu_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_1314_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (13 & 14 TeV). More... | |
| double | eVBF_2_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_DHB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_HB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_Hd_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_HG |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_HQ1_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_Hu_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_2_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (1.96 TeV). More... | |
| double | eVBF_78_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_DHB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_HB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_Hd_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_HG |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_HQ1_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_Hu_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBF_78_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (7 & 8 TeV). More... | |
| double | eVBFint |
| Intrinsic relative theoretical error in VBF production. (Assumed to be constant in energy.) More... | |
| double | eVBFpar |
| Parametric relative theoretical error in VBF production. (Assumed to be constant in energy.) More... | |
| double | eWH_1314_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (13 & 14 TeV). More... | |
| double | eWH_1314_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (13 & 14 TeV). More... | |
| double | eWH_1314_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (13 & 14 TeV). More... | |
| double | eWH_1314_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (13 & 14 TeV). More... | |
| double | eWH_1314_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (13 & 14 TeV). More... | |
| double | eWH_1314_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (13 & 14 TeV). More... | |
| double | eWH_1314_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (13 & 14 TeV). More... | |
| double | eWH_2_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (1.96 TeV). More... | |
| double | eWH_2_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (1.96 TeV). More... | |
| double | eWH_2_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (1.96 TeV). More... | |
| double | eWH_2_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (1.96 TeV). More... | |
| double | eWH_2_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (1.96 TeV). More... | |
| double | eWH_2_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (1.96 TeV). More... | |
| double | eWH_2_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (1.96 TeV). More... | |
| double | eWH_78_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (7 & 8 TeV). More... | |
| double | eWH_78_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (7 & 8 TeV). More... | |
| double | eWH_78_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (7 & 8 TeV). More... | |
| double | eWH_78_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (7 & 8 TeV). More... | |
| double | eWH_78_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (7 & 8 TeV). More... | |
| double | eWH_78_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (7 & 8 TeV). More... | |
| double | eWH_78_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (7 & 8 TeV). More... | |
| double | eWHint |
| Intrinsic relative theoretical error in WH production. (Assumed to be constant in energy.) More... | |
| double | eWHpar |
| Parametric relative theoretical error in WH production. (Assumed to be constant in energy.) More... | |
| double | eZH_1314_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_DHB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_HB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_Hd_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_HQ1_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_Hu_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_1314_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (13 & 14 TeV). More... | |
| double | eZH_2_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_DHB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_HB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_Hd_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_HQ1_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_Hu_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_2_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (1.96 TeV). More... | |
| double | eZH_78_DeltaGF |
| Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_DHB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_DHW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_HB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_Hbox |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_HD |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_Hd_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_HQ1_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_HQ3_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_Hu_11 |
| Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_HW |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZH_78_HWB |
| Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (7 & 8 TeV). More... | |
| double | eZHint |
| Intrinsic relative theoretical error in ZH production. (Assumed to be constant in energy.) More... | |
| double | eZHpar |
| Parametric relative theoretical error in ZH production. (Assumed to be constant in energy.) More... | |
| double | g1_tree |
| The tree level value of the \(U(1)_Y\) gauge coupling contant (at the \(Z\) pole). More... | |
| double | g2_tree |
| The tree level value of the \(SU(2)_L\) gauge coupling contant (at the \(Z\) pole). More... | |
| double | GammaHTotR |
| NP contributions and Total to Higgs width ratio with SM. More... | |
| double | gZdL |
| double | gZdR |
| The tree level value of the \(Z\bar{d}d\) couplings in the SM. More... | |
| double | gZlL |
| double | gZlR |
| The tree level value of the \(Z\ell^+\ell^-\) couplings in the SM. More... | |
| double | gZuL |
| double | gZuR |
| The tree level value of the \(Z\bar{u}u\) couplings in the SM. More... | |
| double | gZvL |
| The tree level value of the \(Z\bar{\nu}\nu\) couplings in the SM. More... | |
| double | Lambda_NP |
| The new physics scale [GeV]. More... | |
| double | lambdaH_tree |
| The SM tree level value of the scalar quartic coupling in the potential. More... | |
| double | LambdaNP2 |
| The square of the new physics scale [GeV \(^2\)]. More... | |
| double | lambZ |
| Independent contribution to aTGC. More... | |
| Matching< NPSMEFTd6Matching, NPSMEFTd6 > | NPSMEFTd6M |
| double | sW2_tree |
| The square of the tree level values for the sine of the weak angle. More... | |
| double | sW_tree |
| The tree level values for the sine of the weak angle. More... | |
| double | UevL |
| The tree level value of the \(W^-\bar{\ell}\nu\) couplings in the SM. (Neglecting PMNS effects.) More... | |
| double | v2 |
| The square of the EW vev. More... | |
| double | v2_over_LambdaNP2 |
| The ratio between the EW vev and the new physics scale, squared \(v^2/\Lambda^2\). More... | |
| double | VudL |
| The tree level value of the \(W^+\bar{u}d\) couplings in the SM. (Neglecting CKM effects.) More... | |
| double | Yukb |
| SM d-quark Yukawas. More... | |
| double | Yukc |
| double | Yukd |
| double | Yuke |
| double | Yukmu |
| double | Yuks |
| double | Yukt |
| SM u-quark Yukawas. More... | |
| double | Yuktau |
| SM lepton Yukawas. More... | |
| double | Yuku |
| Protected Attributes inherited from NPbase | |
| StandardModel | trueSM |
| Protected Attributes inherited from StandardModel | |
| double | A |
| The CKM parameter \(A\) in the Wolfenstein parameterization. More... | |
| double | ale |
| The fine-structure constant \(\alpha\). More... | |
| double | alpha21 |
| double | alpha31 |
| double | AlsMz |
| The strong coupling constant at the Z-boson mass, \(\alpha_s(M_Z)\). More... | |
| bool | bSigmaForAFB |
| bool | bSigmaForR |
| double | dAle5Mz |
| The five-flavour hadronic contribution to the electromagnetic coupling, \(\Delta\alpha_{\mathrm{had}}^{(5)}(M_Z^2)\). More... | |
| double | delGammaZ |
| The theoretical uncertainty in \(\Gamma_Z\), denoted as \(\delta\,\Gamma_Z\), in GeV. More... | |
| double | delMw |
| The theoretical uncertainty in \(M_W\), denoted as \(\delta\,M_W\), in GeV. More... | |
| double | delR0b |
| The theoretical uncertainty in \(R_b^0\), denoted as \(\delta\,R_b^0\). More... | |
| double | delR0c |
| The theoretical uncertainty in \(R_c^0\), denoted as \(\delta\,R_c^0\). More... | |
| double | delR0l |
| The theoretical uncertainty in \(R_l^0\), denoted as \(\delta\,R_l^0\). More... | |
| double | delsigma0H |
| The theoretical uncertainty in \(\sigma_{Hadron}^0\), denoted as \(\delta\,\sigma_{Hadron}^0\) in nb. More... | |
| double | delSin2th_b |
| The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{b}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{b}\). More... | |
| double | delSin2th_l |
| The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{\rm lept}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{\rm lept}\). More... | |
| double | delSin2th_q |
| The theoretical uncertainty in \(\sin^2\theta_{\rm eff}^{q\not = b,t}\), denoted as \(\delta\sin^2\theta_{\rm eff}^{q\not = b,t}\). More... | |
| double | delta |
| double | etab |
| The CKM parameter \(\bar{\eta}\) in the Wolfenstein parameterization. More... | |
| bool | flag_order [orders_EW_size] |
| An array of internal flags controlling the inclusions of higher-order corrections. More... | |
| bool | flagLEP2 [NUMofLEP2RCs] |
| double | gamma |
| \(\gamma \) used as an input for FlagWolfenstein = FALSE More... | |
| double | GF |
| The Fermi constant \(G_\mu\) in \({\rm GeV}^{-2}\). More... | |
| double | lambda |
| The CKM parameter \(\lambda\) in the Wolfenstein parameterization. More... | |
| Particle | leptons [6] |
| An array of Particle objects for the leptons. More... | |
| double | mHl |
| The Higgs mass \(m_h\) in GeV. More... | |
| double | muw |
| A matching scale \(\mu_W\) around the weak scale in GeV. More... | |
| CKM | myCKM |
| An object of type CKM. More... | |
| PMNS | myPMNS |
| double | Mz |
| The mass of the \(Z\) boson in GeV. More... | |
| bool | requireCKM |
| An internal flag to control whether the CKM matrix has to be recomputed. More... | |
| bool | requireYe |
| An internal flag to control whether the charged-lepton Yukawa matrix has to be recomputed. More... | |
| bool | requireYn |
| An internal flag to control whether the neutrino Yukawa matrix has to be recomputed. More... | |
| double | rhob |
| The CKM parameter \(\bar{\rho}\) in the Wolfenstein parameterization. More... | |
| double | s12 |
| double | s13 |
| double | s23 |
| Flavour | SMFlavour |
| An object of type Flavour. More... | |
| Matching< StandardModelMatching, StandardModel > | SMM |
| An object of type Matching. More... | |
| double | Vcb |
| \(\vert V_{cb} \vert \) used as an input for FlagWolfenstein = FALSE More... | |
| double | Vub |
| \(\vert V_{ub} \vert \) used as an input for FlagWolfenstein = FALSE More... | |
| double | Vus |
| \(\vert V_{us} \vert \) used as an input for FlagWolfenstein = FALSE More... | |
| gslpp::matrix< gslpp::complex > | Yd |
| The Yukawa matrix of the down-type quarks. More... | |
| gslpp::matrix< gslpp::complex > | Ye |
| The Yukawa matrix of the charged leptons. More... | |
| gslpp::matrix< gslpp::complex > | Yn |
| The Yukawa matrix of the neutrinos. More... | |
| gslpp::matrix< gslpp::complex > | Yu |
| The Yukawa matrix of the up-type quarks. More... | |
| Protected Attributes inherited from QCD | |
| double | AlsM |
| The strong coupling constant at the mass scale MAls, \(\alpha_s(M_{\alpha_s})\). More... | |
| double | CA |
| double | CF |
| bool | computemt |
| Switch for computing the \(\overline{\mathrm{MS}}\) mass of the top quark. More... | |
| double | dAdA_NA |
| double | dFdA_NA |
| double | dFdF_NA |
| double | FBsoFBd |
| The ratio \( F_{B_s}/F_{B_d} \) necessary to compute \( F_{B_s} \). More... | |
| double | MAls |
| The mass scale in GeV at which the strong coupling measurement is provided. More... | |
| double | mtpole |
| The pole mass of the top quark. More... | |
| double | mub |
| The threshold between five- and four-flavour theory in GeV. More... | |
| double | muc |
| The threshold between four- and three-flavour theory in GeV. More... | |
| double | mut |
| The threshold between six- and five-flavour theory in GeV. More... | |
| double | NA |
| double | Nc |
| The number of colours. More... | |
| Particle | quarks [6] |
| The vector of all SM quarks. More... | |
| bool | requireYd |
| Switch for generating the Yukawa couplings to the down-type quarks. More... | |
| bool | requireYu |
| Switch for generating the Yukawa couplings to the up-type quarks. More... | |
| double | TF |
| Protected Attributes inherited from Model | |
| bool | isSliced |
| A boolean set to true if the current istance is a slice of an extended object. More... | |
| std::map< std::string, boost::reference_wrapper< const double > > | ModelParamMap |
| bool | UpdateError |
| A boolean set to false if update is successful. More... | |
Private Attributes | |
| bool | FlagFlavU3OfX |
| A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients. More... | |
| bool | FlagHiggsSM |
| A boolean flag that is true if including dependence on small variations of the SM parameters (dependence is linearized). Available only in selected Higgs observables. More... | |
| const bool | FlagLeptonUniversal |
| An internal boolean flag that is true if assuming lepton flavour universality. More... | |
| bool | FlagLoopH3d6Quad |
| A boolean flag that is true if including quadratic modifications in the SM loops in Higgs observables due to the dim 6 interactions that contribute to the trilinear Higgs coupling. More... | |
| bool | FlagLoopHd6 |
| A boolean flag that is true if including modifications in the SM loops in Higgs observables due to the dim 6 interactions. More... | |
| bool | FlagPartialQFU |
| A boolean flag that is true if assuming partial quark flavour universality between the 1st and 2nd family in the CHF operators. More... | |
| bool | FlagQuadraticTerms |
| A boolean flag that is true if the quadratic terms in cross sections and widths are switched on. More... | |
| const bool | FlagQuarkUniversal |
| An internal boolean flag that is true if assuming quark flavour universality. More... | |
| bool | FlagRotateCHWCHB |
| A boolean flag that is true if we use as parameters CHWHB_gaga and CHWHB_gagaorth instead of CHW and CHB. More... | |
| bool | FlagUnivOfX |
| A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients and all proportional to the same coefficient (CuH_33 and CuV_33 respectively). More... | |
| gsl_integration_cquad_workspace * | w_WW |
Additional Inherited Members | |
| Public Types inherited from StandardModel | |
| enum | LEP2RCs { Weak = 0, WeakBox, ISR, QEDFSR, QCDFSR, NUMofLEP2RCs } |
| enum | orders_EW { EW1 = 0, EW1QCD1, EW1QCD2, EW2, EW2QCD1, EW3, orders_EW_size } |
| An enumerated type representing perturbative orders of radiative corrections to EW precision observables. More... | |
| Public Types inherited from QCD | |
| enum | lepton { NEUTRINO_1, ELECTRON, NEUTRINO_2, MU, NEUTRINO_3, TAU, NOLEPTON } |
| An enum type for leptons. More... | |
| enum | meson { P_0, P_P, K_0, K_P, D_0, D_P, B_D, B_P, B_S, B_C, PHI, K_star, K_star_P, D_star_P, MESON_END } |
| An enum type for mesons. More... | |
| enum | quark { UP, DOWN, CHARM, STRANGE, TOP, BOTTOM } |
| An enum type for quarks. More... | |
| NPSMEFTd6::NPSMEFTd6 | ( | const bool | FlagLeptonUniversal_in = false, |
| const bool | FlagQuarkUniversal_in = false |
||
| ) |
Constructor.
| [in] | FlagLeptonUniversal_in | an internal boolean flag that is true if assuming lepton flavour universality |
| [in] | FlagQuarkUniversal_in | an internal boolean flag that is true if assuming quark flavour universality |
Definition at line 252 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::AH_f | ( | const double | tau | ) | const |
Fermionic loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings.
\(A^H_f(\tau)=2\tau [1+(1-\tau)f(\tau)]\)
| [in] |
Definition at line 3029 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::AH_W | ( | const double | tau | ) | const |
W loop function entering in the calculation of the effective \(H\gamma\gamma\) coupling.
\(A^H_W(\tau)=-[2+3\tau + 3\tau*(2-\tau) f(\tau)]\)
| [in] |
Definition at line 3034 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::AHZga_f | ( | const double | tau, |
| const double | lambda | ||
| ) | const |
Fermionic loop function entering in the calculation of the effective \(HZ\gamma\) coupling.
| [in] |
Definition at line 3039 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::AHZga_W | ( | const double | tau, |
| const double | lambda | ||
| ) | const |
W loop function entering in the calculation of the effective \(HZ\gamma\) coupling.
| [in] |
Definition at line 3044 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP1 (See code for details.)
Reimplemented from NPbase.
Definition at line 12901 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP2 (See code for details.)
Reimplemented from NPbase.
Definition at line 12928 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP3 (See code for details.)
Reimplemented from NPbase.
Definition at line 12956 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP4 (See code for details.)
Reimplemented from NPbase.
Definition at line 12984 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP5 (See code for details.)
Reimplemented from NPbase.
Definition at line 12990 of file NPSMEFTd6.cpp.
|
virtual |
Auxiliary observable AuxObs_NP6 (See code for details.)
Reimplemented from NPbase.
Definition at line 12996 of file NPSMEFTd6.cpp.
|
virtual |
The branching ratio of the of the Higgs into exotic particles.
Reimplemented from NPbase.
Definition at line 11730 of file NPSMEFTd6.cpp.
|
virtual |
The branching ratio of the of the Higgs into invisible particles.
Reimplemented from NPbase.
Definition at line 11737 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to b\bar{b})\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 9905 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to c\bar{c})\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 9879 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to \gamma\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 9801 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to gg)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 9241 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to \mu^+\mu^-)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 9827 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to \tau^+\tau^-)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 9853 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to invisible)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 11800 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to visible)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 11752 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 9374 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to W j j)\) in the current model and in the Standard Model.
Definition at line 9324 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 9274 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 9299 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 9400 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to WW^*\to 4j)\) in the current model and in the Standard Model.
Definition at line 9349 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to WW)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 9267 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.
Definition at line 9645 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 9688 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Z\gamma\to ee\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 9779 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Z\gamma\to ll\gamma)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 9764 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Z\gamma\to \mu\mu\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 9790 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Z\gamma)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 9738 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 9430 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model.
Definition at line 9605 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to Z\nu\nu)\) in the current model and in the Standard Model.
Definition at line 9555 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 2e 2\mu)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 9505 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.
Definition at line 9670 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 4e)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 9480 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 9713 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 9455 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 9530 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model.
Definition at line 9630 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model.
Definition at line 9580 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the Br \((H\to ZZ)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 9425 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{EB,UB,DB}\) corresponding to particle f.
| [in] | f | a lepton or quark |
Definition at line 2327 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{UG,DG}\) corresponding to particle f.
| [in] | f | a lepton or quark |
Definition at line 2275 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{EH,UH,DH}\) corresponding to particle f.
| [in] | f | a lepton or quark |
Definition at line 2249 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{EW,UW,DW}\) corresponding to particle f.
| [in] | f | a lepton or quark |
Definition at line 2301 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(c_{\gamma\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 12870 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(c_{gg}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 12880 of file NPSMEFTd6.cpp.
|
virtual |
A method to check if all the mandatory parameters for NPSMEFTd6 have been provided in model initialization.
| [in] | DPars | a map of the parameters that are being updated in the Monte Carlo run (including parameters that are varied and those that are held constant) |
Reimplemented from StandardModel.
Definition at line 2087 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(1)}\) corresponding to particle F.
| [in] | F | a lepton or quark |
Definition at line 2172 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{HL,HQ}^{(3)}\) corresponding to particle F.
| [in] | F | a lepton or quark |
Definition at line 2190 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{HE,HU,HD}\) corresponding to particle f.
| [in] | f | a lepton or quark |
Definition at line 2208 of file NPSMEFTd6.cpp.
|
protected |
The diagonal entry of the dimension-6 operator coefficient \(C_{Hud}\) corresponding to particle f.
| [in] | u | a quark |
Definition at line 2234 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLL_bottom | ( | ) | const |
Definition at line 13296 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLL_charm | ( | ) | const |
Definition at line 13286 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLL_down | ( | ) | const |
Definition at line 13281 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLL_mu | ( | ) | const |
Definition at line 13266 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLL_strange | ( | ) | const |
Definition at line 13291 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLL_tau | ( | ) | const |
Definition at line 13271 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLL_up | ( | ) | const |
Definition at line 13276 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLR_bottom | ( | ) | const |
Definition at line 13331 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLR_charm | ( | ) | const |
Definition at line 13321 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLR_down | ( | ) | const |
Definition at line 13316 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLR_mu | ( | ) | const |
Definition at line 13301 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLR_strange | ( | ) | const |
Definition at line 13326 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLR_tau | ( | ) | const |
Definition at line 13306 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CLR_up | ( | ) | const |
Definition at line 13311 of file NPSMEFTd6.cpp.
|
virtual |
The ratio of the \(\Gamma(H)\) in the current model and in the Standard Model.
Reimplemented from NPbase.
Definition at line 9931 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRL_bottom | ( | ) | const |
Definition at line 13366 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRL_charm | ( | ) | const |
Definition at line 13356 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRL_down | ( | ) | const |
Definition at line 13351 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRL_mu | ( | ) | const |
Definition at line 13336 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRL_strange | ( | ) | const |
Definition at line 13361 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRL_tau | ( | ) | const |
Definition at line 13341 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRL_up | ( | ) | const |
Definition at line 13346 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRR_bottom | ( | ) | const |
Definition at line 13402 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRR_charm | ( | ) | const |
Definition at line 13392 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRR_down | ( | ) | const |
Definition at line 13387 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRR_mu | ( | ) | const |
Definition at line 13371 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRR_strange | ( | ) | const |
Definition at line 13397 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRR_tau | ( | ) | const |
Definition at line 13376 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::CRR_up | ( | ) | const |
Definition at line 13382 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(c_{z\Box}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 12834 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(c_{z\gamma}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 12858 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(c_{zz}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 12846 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the electromagnetic constant at zero momentum, \(\delta \alpha(0)/\alpha(0)\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2476 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the electromagnetic constant at zero momentum, \((\delta \alpha(0)/\alpha(0))^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2482 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the electromagnetic constant at the Z pole, \(\delta \alpha(M_Z^2)/\alpha(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2465 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the electromagnetic constant at the Z pole, \((\delta \alpha(M_Z^2)/\alpha(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2471 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the strong coupling constant at the Z pole, \(\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2)\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2487 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the strong coupling constant at the Z pole, \((\delta \alpha_S(M_Z^2)/\alpha_S(M_Z^2))^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2493 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(\delta c_z\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 12824 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\mu\nu}^\dagger W^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 2692 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 2730 of file NPSMEFTd6.cpp.
|
virtual |
The full new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} F^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
Reimplemented from NPbase.
Definition at line 2735 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} Z^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 2713 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the anomalous triple gauge coupling \(g_{1,Z}\).
Reimplemented from NPbase.
Definition at line 12190 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\nu}^\dagger \partial^\mu W^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 2697 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu F^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 2815 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\nu} \partial^\mu Z^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 2718 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H W_{\mu}^\dagger W^{\mu}\).
Reimplemented from NPbase.
Definition at line 2702 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu} Z^{\mu}\).
Reimplemented from NPbase.
Definition at line 2723 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltag3G | ( | ) | const |
The new physics contribution to the coupling of the effective interaction \(f_{ABC} G_{\mu\nu}^A G_{\nu\rho}^B G_{\rho\mu}^C\).
Definition at line 2975 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::deltaG_Aff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 2968 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::deltaG_Gff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 2954 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\).
Reimplemented from NPbase.
Definition at line 2820 of file NPSMEFTd6.cpp.
|
virtual |
The full new physics contribution to the coupling of the effective interaction \(H F_{\mu\nu} F^{\mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
Reimplemented from NPbase.
Definition at line 2825 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::deltaG_hAff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H A_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 2947 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H f\bar{f}\).
| [in] | p | a lepton or quark |
Reimplemented from NPbase.
Definition at line 2878 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::deltaG_hGff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 2933 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\).
Reimplemented from NPbase.
Definition at line 2665 of file NPSMEFTd6.cpp.
|
virtual |
The full new physics contribution to the coupling of the effective interaction \(H G_{\mu\nu}^AG^{A \mu\nu}\), including new local terms and modifications on the SM-loops. Normalized to the SM value.
Reimplemented from NPbase.
Definition at line 2670 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the Higgs self-coupling \( H H H\). Normalized to the SM value.
Reimplemented from NPbase.
Definition at line 2892 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::deltaG_hZff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 2940 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::deltaG_Zff | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(Z_{\mu\nu} \bar{f}\sigmma^{\mu\nu} f\).
| [in] | p | a lepton or quark |
Definition at line 2961 of file NPSMEFTd6.cpp.
|
virtual |
New physics contribution to the neutral-current axial-vector coupling \(g_A^f\).
| [in] | f | a lepton or quark |
Reimplemented from NPbase.
Definition at line 2605 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the total decay width of the \(W\) boson, \(\delta \Gamma_W\).
Reimplemented from NPbase.
Definition at line 2558 of file NPSMEFTd6.cpp.
The new physics contribution to the decay width of the \(W\) boson into a given fermion pair, \(\delta \Gamma_Z^{f}\).
| [in] | fi | a lepton or quark |
| [in] | fj | a lepton or quark |
Reimplemented from NPbase.
Definition at line 2524 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHbbRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11680 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHbbRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11720 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHccRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11615 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHccRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11655 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHgagaRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11434 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHgagaRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11484 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHggRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients.
Definition at line 10005 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHggRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 10040 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHmumuRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11510 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHmumuRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11536 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHtautauRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11562 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHtautauRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11589 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWffRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 10347 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWffRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 10378 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWjjRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 10231 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWjjRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 10261 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWlvRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 10114 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWlvRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Wl\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 10144 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWW2l2vRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 10170 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWW2l2vRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 10205 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWW4fRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 10404 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWW4fRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 10448 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWW4jRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 10287 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWW4jRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 10321 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWWRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 10066 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHWWRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 10086 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZddRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11141 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZddRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z d d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11174 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZeeRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 10581 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZeeRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 10616 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZffRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11200 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZffRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z ff)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11237 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZgaRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11349 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZgaRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11408 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZllRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 10522 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZllRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 10555 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZmumuRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 10642 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZmumuRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 10677 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZuuRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11082 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZuuRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z u u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11115 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZvvRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 10961 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZvvRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 10993 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZ2e2muRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 10836 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZ2e2muRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 10873 of file NPSMEFTd6.cpp.
|
inline |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 2361 of file NPSMEFTd6.h.
| double NPSMEFTd6::deltaGammaHZZ4dRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
| double NPSMEFTd6::deltaGammaHZZ4eRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 10773 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZ4eRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 10810 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZ4fRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11263 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZ4fRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11323 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZ4lRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 10703 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZ4lRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 10747 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZ4muRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 10898 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZ4muRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 10935 of file NPSMEFTd6.cpp.
|
inline |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 2344 of file NPSMEFTd6.h.
| double NPSMEFTd6::deltaGammaHZZ4uRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
| double NPSMEFTd6::deltaGammaHZZ4vRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 11019 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZ4vRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 11056 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZRatio1 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are linear in the effective Lagrangian coefficients.)
Definition at line 10474 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGammaHZZRatio2 | ( | ) | const |
The new physics contribution to the ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model. (Only terms that are quadratic in the effective Lagrangian coefficients.)
Definition at line 10494 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are linear in the effective Lagrangian coefficients.
Definition at line 9948 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the ratio of the \(\Gamma(H)\) in the current model and in the Standard Model. Only terms that are quadratic in the effective Lagrangian coefficients.
Definition at line 9970 of file NPSMEFTd6.cpp.
|
virtual |
New physics contribution to the Fermi constant.
The new physics contribution \(\Delta G\) is defined as
\[ G_\mu = G_{\mu,\mathrm{SM}}(1+\Delta G)\,, \]
where \(G_\mu\) is the experimental value measured through muon decays, and \(G_{\mu,\mathrm{SM}}\) is the Fermi constant in the SM.
Reimplemented from NPbase.
Definition at line 2356 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGL_f | ( | const Particle | p | ) | const |
New physics contribution to the neutral-current left-handed coupling \(g_L^f\).
| [in] | f | a lepton or quark |
Definition at line 2610 of file NPSMEFTd6.cpp.
|
virtual |
New physics contribution to the charged current coupling \(W_\mu \bar{f_L}\gamma^mu f_L\).
| [in] | pbar | a lepton or quark |
| [in] | p | a lepton or quark |
Reimplemented from NPbase.
Definition at line 2641 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::deltaGL_Wffh | ( | const Particle | pbar, |
| const Particle | p | ||
| ) | const |
The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_L}\gamma^mu f_L\).
| [in] | pbar | a lepton or quark |
| [in] | p | a lepton or quark |
Definition at line 2901 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGL_Zffh | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_L}\gamma^mu f_L\).
| [in] | p | a lepton or quark |
Definition at line 2919 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the muon decay constant, \(\delta G_\mu/G_\mu\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2454 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the muon decay constant, \((\delta G_\mu/G_\mu)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2460 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGR_f | ( | const Particle | p | ) | const |
New physics contribution to the neutral-current right-handed coupling \(g_R^f\).
| [in] | f | a lepton or quark |
Definition at line 2625 of file NPSMEFTd6.cpp.
|
virtual |
New physics contribution to the charged current coupling \(W_\mu \bar{f_R}\gamma^mu f_R\).
| [in] | pbar | a lepton or quark |
| [in] | p | a lepton or quark |
Reimplemented from NPbase.
Definition at line 2656 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::deltaGR_Wffh | ( | const Particle | pbar, |
| const Particle | p | ||
| ) | const |
The new physics contribution to the coupling of the effective interaction \(H W_\mu \bar{f_R}\gamma^mu f_R\).
| [in] | pbar | a lepton or quark |
| [in] | p | a lepton or quark |
Definition at line 2910 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::deltaGR_Zffh | ( | const Particle | p | ) | const |
The new physics contribution to the coupling of the effective interaction \(H Z_\mu \bar{f_R}\gamma^mu f_R\).
| [in] | p | a lepton or quark |
Definition at line 2927 of file NPSMEFTd6.cpp.
|
virtual |
New physics contribution to the neutral-current vector coupling \(g_V^f\).
| [in] | f | a lepton or quark |
Reimplemented from NPbase.
Definition at line 2600 of file NPSMEFTd6.cpp.
|
virtual |
The relative NP corrections to the width of the \(W\) boson, \(\delta \Gamma_W/\Gamma_W\).
Definition at line 2576 of file NPSMEFTd6.cpp.
|
virtual |
The relative NP corrections to the width of the \(W\) boson squared, \((\delta \Gamma_W/\Gamma_W)^2\).
Definition at line 2581 of file NPSMEFTd6.cpp.
|
virtual |
The relative NP corrections to the width of the \(Z\) boson, \(\delta \Gamma_Z/\Gamma_Z\).
Definition at line 2588 of file NPSMEFTd6.cpp.
|
virtual |
The relative NP corrections to the width of the \(Z\) boson squared, \((\delta \Gamma_Z/\Gamma_Z)^2\).
Definition at line 2593 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the anomalous triple gauge coupling \(\kappa_{\gamma}\).
Reimplemented from NPbase.
Definition at line 12207 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(b\) quark, \(\delta m_b/m_b\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2421 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(b\) quark squared, \((\delta m_b/m_b)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2427 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(c\) quark, \(\delta m_c/m_c\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2432 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(c\) quark squared, \((\delta m_c/m_c)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2438 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(H\) boson, \(\delta M_H/M_H\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2399 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(H\) boson squared, \((\delta M_H/M_H)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2405 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(t\) quark, \(\delta m_t/m_t\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2410 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(t\) quark squared, \((\delta m_t/m_t)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2416 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(\tau\) lepton, \(\delta m_\tau/m_\tau\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2443 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(\tau\) lepton squared, \((\delta m_\tau/m_\tau)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2449 of file NPSMEFTd6.cpp.
|
virtual |
The relative NP corrections to the mass of the \(W\) boson, \(\delta M_W/M_W\).
Definition at line 2509 of file NPSMEFTd6.cpp.
|
virtual |
The relative NP corrections to the mass of the \(W\) boson squared, \((\delta M_W/M_W)^2\).
Definition at line 2517 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(Z\) boson, \(\delta M_Z/M_Z\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2388 of file NPSMEFTd6.cpp.
|
virtual |
The relative correction to the mass of the \(Z\) boson squared, \((\delta M_Z/M_Z)^2\), with respect to ref. point used in the SM calculation of Higgs observables.
Definition at line 2394 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(\delta y_b\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 12780 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(\delta y_c\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 12802 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(\delta y_\mu\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 12813 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(\delta y_t\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 12769 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(\delta y_\tau\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 12791 of file NPSMEFTd6.cpp.
|
virtual |
The differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\), as a function of the \(W\) polar angle.
Reimplemented from NPbase.
Definition at line 12233 of file NPSMEFTd6.cpp.
|
virtual |
The integral of differential distribution for \(e^+ e^- \to W^+ W^- \to jj \ell \nu\), with \(\ell= e, \mu\) in a given bin of the \(W\) polar angle.
< Gsl integral variable
< Gsl integral variable
< Gsl integral variable
Reimplemented from NPbase.
Definition at line 12532 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::f_triangle | ( | const double | tau | ) | const |
Loop function entering in the calculation of the effective \(Hgg\) and \(H\gamma\gamma\) couplings.
| [in] |
Definition at line 2985 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::g_triangle | ( | const double | tau | ) | const |
Loop function entering in the calculation of the effective \(HZ\gamma\) coupling.
| [in] |
Definition at line 2997 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHbbRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to bb)\) in the current model and in the Standard Model.
Definition at line 11665 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHccRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to cc)\) in the current model and in the Standard Model.
Definition at line 11599 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHgagaRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to \gamma\gamma)\) in the current model and in the Standard Model.
Definition at line 11418 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHggRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to gg)\) in the current model and in the Standard Model.
Definition at line 9989 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHmumuRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to \mu\mu)\) in the current model and in the Standard Model.
Definition at line 11494 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHtautauRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to \tau\tau)\) in the current model and in the Standard Model.
Definition at line 11546 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHWffRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to W f f)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 10331 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHWjjRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to W j j)\) in the current model and in the Standard Model.
Definition at line 10215 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHWlvRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to W l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Definition at line 10098 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHWW2l2vRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to WW^*\to l\nu l\nu)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Definition at line 10154 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHWW4fRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to WW^*\to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 10388 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHWW4jRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to WW^*\to 4j)\) in the current model and in the Standard Model.
Definition at line 10271 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHWWRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to WW)\) in the current model and in the Standard Model.
Definition at line 10050 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZddRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Zd d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.
Definition at line 11125 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZeeRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Zee)\) in the current model and in the Standard Model.
Definition at line 10565 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZffRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Zff)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 11184 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZgaRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Z\gamma)\) in the current model and in the Standard Model.
Definition at line 11333 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZllRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Zll)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Definition at line 10506 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZmumuRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Z\mu\mu)\) in the current model and in the Standard Model.
Definition at line 10626 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZuuRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Zu u)\) ( \(u=u,c \)) in the current model and in the Standard Model.
Definition at line 11066 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZvvRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to Z\nu\nu)\) in the current model and in the Standard Model.
Definition at line 10945 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZZ2e2muRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to ZZ* \to 2e2\mu)\) in the current model and in the Standard Model.
Definition at line 10820 of file NPSMEFTd6.cpp.
|
inline |
The ratio of the \(\Gamma(H\to ZZ* \to 4 d)\) ( \(d=d,s,b \)) in the current model and in the Standard Model.
Definition at line 2153 of file NPSMEFTd6.h.
| double NPSMEFTd6::GammaHZZ4eRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to ZZ* \to 4e)\) in the current model and in the Standard Model.
Definition at line 10757 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZZ4fRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to ZZ* \to 4f)\), with \(f\) any fermion, in the current model and in the Standard Model.
Definition at line 11247 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZZ4lRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to ZZ* \to 4l)\) ( \(l=e,\mu \)) in the current model and in the Standard Model.
Definition at line 10687 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZZ4muRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to ZZ* \to 4\mu)\) in the current model and in the Standard Model.
Definition at line 10882 of file NPSMEFTd6.cpp.
|
inline |
The ratio of the \(\Gamma(H\to ZZ* \to 4 u)\) ( \(u=u,c \)) in the current model and in the Standard Model.
Definition at line 2138 of file NPSMEFTd6.h.
| double NPSMEFTd6::GammaHZZ4vRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to ZZ* \to 4\nu)\) in the current model and in the Standard Model.
Definition at line 11003 of file NPSMEFTd6.cpp.
| double NPSMEFTd6::GammaHZZRatio | ( | ) | const |
The ratio of the \(\Gamma(H\to ZZ)\) in the current model and in the Standard Model.
Definition at line 10458 of file NPSMEFTd6.cpp.
A partial decay width of the \(W\) boson decay into a SM fermion pair.
| [in] | fi | a lepton or quark |
| [in] | fj | a lepton or quark |
Reimplemented from NPbase.
Definition at line 2553 of file NPSMEFTd6.cpp.
|
virtual |
The total width of the \(W\) boson, \(\Gamma_W\).
Reimplemented from NPbase.
Definition at line 2571 of file NPSMEFTd6.cpp.
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inline |
|
inlinevirtual |
A method to get the Matching object for this model.
Reimplemented from StandardModel.
Definition at line 829 of file NPSMEFTd6.h.
| gslpp::complex NPSMEFTd6::I_triangle_1 | ( | const double | tau, |
| const double | lambda | ||
| ) | const |
Loop function entering in the calculation of the effective \(HZ\gamma\) coupling.
| [in] |
Definition at line 3009 of file NPSMEFTd6.cpp.
| gslpp::complex NPSMEFTd6::I_triangle_2 | ( | const double | tau, |
| const double | lambda | ||
| ) | const |
Loop function entering in the calculation of the effective \(HZ\gamma\) coupling.
| [in] |
Definition at line 3020 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{A,eff}=\sqrt{\Gamma_{HAA}/\Gamma_{HAA}^{SM}}\).
Reimplemented from NPbase.
Definition at line 12755 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{b,eff}=\sqrt{\Gamma_{Hbb}/\Gamma_{Hbb}^{SM}}\).
Reimplemented from NPbase.
Definition at line 12735 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{c,eff}=\sqrt{\Gamma_{Hcc}/\Gamma_{Hcc}^{SM}}\).
Reimplemented from NPbase.
Definition at line 12730 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{G,eff}=\sqrt{\Gamma_{HGG}/\Gamma_{HGG}^{SM}}\).
Reimplemented from NPbase.
Definition at line 12740 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{\mu,eff}=\sqrt{\Gamma_{H\mu\mu}/\Gamma_{H\mu\mu}^{SM}}\).
Reimplemented from NPbase.
Definition at line 12720 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{\tau,eff}=\sqrt{\Gamma_{H\tau\tau}/\Gamma_{H\tau\tau}^{SM}}\).
Reimplemented from NPbase.
Definition at line 12725 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{W,eff}=\sqrt{\Gamma_{HWW}/\Gamma_{HWW}^{SM}}\).
Reimplemented from NPbase.
Definition at line 12750 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{ZA,eff}=\sqrt{\Gamma_{HZA}/\Gamma_{HZA}^{SM}}\).
Reimplemented from NPbase.
Definition at line 12760 of file NPSMEFTd6.cpp.
|
virtual |
The effective coupling \(\kappa_{Z,eff}=\sqrt{\Gamma_{HZZ}/\Gamma_{HZZ}^{SM}}\).
Reimplemented from NPbase.
Definition at line 12745 of file NPSMEFTd6.cpp.
|
virtual |
The new physics contribution to the anomalous triple gauge coupling \(\lambda_{Z}\).
Reimplemented from NPbase.
Definition at line 12221 of file NPSMEFTd6.cpp.
|
virtual |
The Higgs-basis coupling \(\lambda_{z}\). (See LHCHXSWG-INT-2015-001 document.) Note that the Lagrangian definition of the Higgs-basis parameters coincides with the one of some of the \(g_i, \delta g_i\) couplings defined above. In the Higgs basis, however, one uses the freedom to perform certain field redefinitions and operations to demand that the mass eigenstate Lagrangian has specific features. (See pag. 5,6 in the reference.) Therefore, the actual expression in terms of dim 6 coefficients may differ from the one for \(g_i, \delta g_i\).
Reimplemented from NPbase.
Definition at line 12890 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 3754 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{e^+e^- \to H\nu\bar{\nu}}\) between the \( e^+e^- \to H\nu\bar{\nu} \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 4089 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 8422 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eettH}\) between the \( e^{+}e^{-}\to t\bar{t} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 8619 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 3452 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeWBF}\) between the \( e^{+}e^{-}\to \nu\bar{\nu} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 3745 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 5073 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZBF}\) between the \( e^{+}e^{-}\to e^{+}e^{-} H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 5387 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZH}\) between the \(e^{+}e^{-}\to ZH\) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 6895 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZH}\) between the \( e^{+}e^{-}\to ZH \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 7252 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 7207 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZH, Z \to e^+ e^-, \mu^+ \mu^-}\) between the \( e^{+}e^{-}\to ZH, Z \to e^+ e^-, \mu^+ \mu^- \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 8194 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 7227 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{eeZH, Z \to q \bar{q}}\) between the \( e^{+}e^{-}\to ZH, Z \to q \bar{q} \) associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV, Pol_em and Pol_ep are the polarization of electrons and positrons, respectively |
Reimplemented from NPbase.
Definition at line 8214 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{epWBF}\) between the \( e^{-} p\to \nu j H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 6330 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{epZBF}\) between the \( e^{-} p\to e^{-} j H \) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 6418 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH}\) between the gluon-gluon fusion Higgs production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 3057 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,bb}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12152 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,\gamma\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11864 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggHH}\) between the gluon-gluon fusion di-Higgs production cross-section in the current model and in the Standard Model. (From arXiv: 1502.00539 [hpe-ph].)
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 3113 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,\mu\mu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12080 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH+ttH}\) between the sum of gluon-gluon fusion and t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 8408 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,\tau\tau}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12116 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,WW}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12008 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,WW\to 2l2\nu}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12044 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,Z\gamma}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11900 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,ZZ}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11936 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ggH,ZZ\to 4l}\) between the gluon-gluon fusion Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11972 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{\mu\mu H}\) between the \(\sigma(\mu \mu \to H)}\) production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 9221 of file NPSMEFTd6.cpp.
|
virtual |
The number of events in \( p p \to WZ\) in a given \(p_{TV}\) bin, normalized to the SM prediction. From arXiv: 1712.01310 [hep-ph] and private communication. Implemented only in NPSMEFTd6 class.
Reimplemented from NPbase.
Definition at line 12623 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH}\) between the t-tbar-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 8267 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,bb}\) between the ttH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12182 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,\gamma\gamma}\) between the ttH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11894 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,\mu\mu}\) between the ttH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12110 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,\tau\tau}\) between the ttH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12146 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,WW}\) between the ttH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12038 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,WW\to 2l2\nu}\) between the ttH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12074 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\sigma(ttH)/\sigma(ttZ)\) in the \(H,Z\to b\bar{b}\) channel in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11808 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,Z\gamma}\) between the ttH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11930 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,ZZ}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11966 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ttH,ZZ\to 4l}\) between the ttH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12002 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF}\) between the vector-boson fusion Higgs production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 3192 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF+\gamma}\) between the vector-boson fusion Higgs production cross-section in association with a hard photon in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 3407 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,bb}\) between the VBF Higgs production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12158 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,\gamma\gamma}\) between the VBF Higgs production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11870 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,\mu\mu}\) between the VBF Higgs production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12086 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,\tau\tau}\) between the VBF Higgs production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12122 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,WW}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12014 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,WW\to 2l2\nu}\) between the VBF Higgs production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12050 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,Z\gamma}\) between the VBF Higgs production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11906 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,ZZ}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11942 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF,ZZ\to 4l}\) between the VBF Higgs production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11978 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VBF+VH}\) between the sum of VBF and WH+ZH associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 8252 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH}\) between the WH+ZH associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 8239 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,bb}\) between the VH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12176 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,\gamma\gamma}\) between the VH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11888 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,\mu\mu}\) between the VH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12104 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,\tau\tau}\) between the VH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12140 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,WW}\) between the VH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12032 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,WW\to 2l2\nu}\) between the VH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12068 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,Z\gamma}\) between the VH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11924 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,ZZ}\) between the VH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11960 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{VH,ZZ\to 4l}\) between the VH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11996 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH}\) between the W-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 6530 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,bb}\) between the WH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12170 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,\gamma\gamma}\) between the WH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11882 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,\mu\mu}\) between the WH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12098 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,\tau\tau}\) between the WH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12134 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,WW}\) between the WH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12026 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,WW\to 2l2\nu}\) between the WH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12062 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,Z\gamma}\) between the WH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11918 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,ZZ}\) between the WH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11954 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{WH,ZZ\to 4l}\) between the WH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11990 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH}\) between the Z-Higgs associated production cross-section in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 6699 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,bb}\) between the ZH production cross-section with subsequent decay into \(bb\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12164 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,\gamma\gamma}\) between the ZH production cross-section with subsequent decay into 2 photons in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11876 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,\mu\mu}\) between the ZH production cross-section with subsequent decay into \(\mu\mu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12092 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,\tau\tau}\) between the ZH production cross-section with subsequent decay into \(\tau\tau\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12128 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,WW}\) between the ZH production cross-section with subsequent decay into \(W W^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12020 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,WW\to 2l2\nu}\) between the ZH production cross-section with subsequent decay into \(W W^*\to 2l2\nu\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 12056 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,Z\gamma}\) between the ZH production cross-section with subsequent decay into \(Z \gamma\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11912 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,ZZ}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11948 of file NPSMEFTd6.cpp.
|
virtual |
The ratio \(\mu_{ZH,ZZ\to 4l}\) between the ZH production cross-section with subsequent decay into \(Z Z^*\to 4l\) in the current model and in the Standard Model.
| [in] | sqrt_s | the center-of-mass energy in TeV |
Reimplemented from NPbase.
Definition at line 11984 of file NPSMEFTd6.cpp.
|
virtual |
The mass of the \(W\) boson, \(M_W\).
Reimplemented from NPbase.
Definition at line 2501 of file NPSMEFTd6.cpp.
|
virtual |
The oblique parameter \(S\). (Simplified implementation. Contribution only from \(O_{HWB}\).)
Reimplemented from NPbase.
Definition at line 2361 of file NPSMEFTd6.cpp.
|
virtual |
The oblique parameter \(T\). (Simplified implementation. Contribution only from \(O_{HD}\).)
Reimplemented from NPbase.
Definition at line 2366 of file NPSMEFTd6.cpp.
|
virtual |
The oblique parameter \(U\).
Reimplemented from NPbase.
Definition at line 2371 of file NPSMEFTd6.cpp.
|
virtual |
The oblique parameter \(W\). (Simplified implementation. Contribution only from \(O_{2W}\).)
Reimplemented from NPbase.
Definition at line 2376 of file NPSMEFTd6.cpp.
|
virtual |
The oblique parameter \(Y\). (Simplified implementation. Contribution only from \(O_{2B}\).)
Reimplemented from NPbase.
Definition at line 2381 of file NPSMEFTd6.cpp.
|
virtual |
The post-update method for NPSMEFTd6.
This method runs all the procedures that are need to be executed after the model is successfully updated.
Reimplemented from NPbase.
Definition at line 789 of file NPSMEFTd6.cpp.
|
virtual |
The direction constrained by \( p p \to Z H\) in the boosted regime, \(g_p^Z\). From arXiv:1807.01796 and the contribution to FCC CDR Vol 1. Implemented only in NPSMEFTd6 class.
Reimplemented from NPbase.
Definition at line 12587 of file NPSMEFTd6.cpp.
|
virtual |
A method to set a flag of NPSMEFTd6.
| [in] | name | name of a model flag |
| [in] | value | the boolean to be assigned to the flag specified by name |
Reimplemented from StandardModel.
Definition at line 2135 of file NPSMEFTd6.cpp.
|
protectedvirtual |
A method to set the value of a parameter of the model.
| [in] | name | name of a model parameter |
| [in] | value | the value to be assigned to the parameter specified by name |
Reimplemented from StandardModel.
Definition at line 990 of file NPSMEFTd6.cpp.
|
virtual |
Total \(e^+ e^- \to W^+ W^- \to jj \ell \nu\) cross section in pb, with \(\ell= e, \mu\).
Reimplemented from NPbase.
Definition at line 12577 of file NPSMEFTd6.cpp.
|
protected |
The em constant at Mz.
Definition at line 3802 of file NPSMEFTd6.h.
|
protected |
The branching ratio of exotic (not invisible) Higgs decays.
Definition at line 3794 of file NPSMEFTd6.h.
|
protected |
The branching ratio of invisible Higgs decays.
Definition at line 3793 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{2W}\).
Definition at line 3431 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{2B}\).
Definition at line 3432 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{11}\) (imaginary part).
Definition at line 3549 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{11}\) (real part).
Definition at line 3543 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{12}\) (imaginary part).
Definition at line 3550 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{12}\) (real part).
Definition at line 3544 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{13}\) (imaginary part).
Definition at line 3551 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{13}\) (real part).
Definition at line 3545 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{22}\) (imaginary part).
Definition at line 3552 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{22}\) (real part).
Definition at line 3546 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{23}\) (imaginary part).
Definition at line 3553 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{23}\) (real part).
Definition at line 3547 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{33}\) (imaginary part).
Definition at line 3554 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{dH})_{33}\) (real part).
Definition at line 3548 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{DHB}\).
Definition at line 3438 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{DHW}\).
Definition at line 3439 of file NPSMEFTd6.h.
|
protected |
Definition at line 3611 of file NPSMEFTd6.h.
|
protected |
Definition at line 3612 of file NPSMEFTd6.h.
|
protected |
Definition at line 3614 of file NPSMEFTd6.h.
|
protected |
Definition at line 3615 of file NPSMEFTd6.h.
|
protected |
Definition at line 3613 of file NPSMEFTd6.h.
|
protected |
Definition at line 3612 of file NPSMEFTd6.h.
|
protected |
Definition at line 3614 of file NPSMEFTd6.h.
|
protected |
Definition at line 3615 of file NPSMEFTd6.h.
|
protected |
Definition at line 3613 of file NPSMEFTd6.h.
|
protected |
Definition at line 3614 of file NPSMEFTd6.h.
|
protected |
Definition at line 3615 of file NPSMEFTd6.h.
|
protected |
Definition at line 3604 of file NPSMEFTd6.h.
|
protected |
Definition at line 3605 of file NPSMEFTd6.h.
|
protected |
Definition at line 3606 of file NPSMEFTd6.h.
|
protected |
Definition at line 3605 of file NPSMEFTd6.h.
|
protected |
Definition at line 3606 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{11}\) (imaginary part).
Definition at line 3525 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{11}\) (real part).
Definition at line 3519 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{12}\) (imaginary part).
Definition at line 3526 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{12}\) (real part).
Definition at line 3520 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{13}\) (imaginary part).
Definition at line 3527 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{13}\) (real part).
Definition at line 3521 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{22}\) (imaginary part).
Definition at line 3528 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{22}\) (real part).
Definition at line 3522 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{23}\) (imaginary part).
Definition at line 3529 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{23}\) (real part).
Definition at line 3523 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{33}\) (imaginary part).
Definition at line 3530 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{eH})_{33}\) (real part).
Definition at line 3524 of file NPSMEFTd6.h.
|
protected |
Definition at line 3607 of file NPSMEFTd6.h.
|
protected |
Definition at line 3608 of file NPSMEFTd6.h.
|
protected |
Definition at line 3609 of file NPSMEFTd6.h.
|
protected |
Definition at line 3608 of file NPSMEFTd6.h.
|
protected |
Definition at line 3610 of file NPSMEFTd6.h.
|
protected |
Definition at line 3609 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{G}\).
Definition at line 3429 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{H}\).
Definition at line 3443 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{HB}\).
Definition at line 3435 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{H\Box}\).
Definition at line 3442 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{HD}\).
Definition at line 3441 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{11}\).
Definition at line 3498 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{12}\) (imaginary part).
Definition at line 3504 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{12}\) (real part).
Definition at line 3499 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{13}\) (imaginary part).
Definition at line 3505 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{13}\) (real part).
Definition at line 3500 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{22}\).
Definition at line 3501 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{23}\) (imaginary part).
Definition at line 3506 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{23}\) (real part).
Definition at line 3502 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hd})_{33}\).
Definition at line 3503 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{11}\).
Definition at line 3462 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{12}\) (imaginary part).
Definition at line 3468 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{12}\) (real part).
Definition at line 3463 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{13}\) (imaginary part).
Definition at line 3469 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{13}\) (real part).
Definition at line 3464 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{22}\).
Definition at line 3465 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{23}\) (imaginary part).
Definition at line 3470 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{23}\) (real part).
Definition at line 3466 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{He})_{33}\).
Definition at line 3467 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{HG}\).
Definition at line 3433 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{11}\).
Definition at line 3444 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (imaginary part).
Definition at line 3450 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{12}\) (real part).
Definition at line 3445 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (imaginary part).
Definition at line 3451 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{13}\) (real part).
Definition at line 3446 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{22}\).
Definition at line 3447 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (imaginary part).
Definition at line 3452 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{23}\) (real part).
Definition at line 3448 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(1)})_{33}\).
Definition at line 3449 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{11}\).
Definition at line 3453 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part).
Definition at line 3459 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{12}\) (real part).
Definition at line 3454 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part).
Definition at line 3460 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{13}\) (real part).
Definition at line 3455 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{22}\).
Definition at line 3456 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part).
Definition at line 3461 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{23}\) (real part).
Definition at line 3457 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HL}^{(3)})_{33}\).
Definition at line 3458 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{11}\).
Definition at line 3471 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (imaginary part).
Definition at line 3477 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{12}\) (real part).
Definition at line 3472 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (imaginary part).
Definition at line 3478 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{13}\) (real part).
Definition at line 3473 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{22}\).
Definition at line 3474 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (imaginary part).
Definition at line 3479 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{23}\) (real part).
Definition at line 3475 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(1)})_{33}\).
Definition at line 3476 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{11}\).
Definition at line 3480 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (imaginary part).
Definition at line 3486 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{12}\) (real part).
Definition at line 3481 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (imaginary part).
Definition at line 3487 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{13}\) (real part).
Definition at line 3482 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{22}\).
Definition at line 3483 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (imaginary part).
Definition at line 3488 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{23}\) (real part).
Definition at line 3484 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{HQ}^{(3)})_{33}\).
Definition at line 3485 of file NPSMEFTd6.h.
|
protected |
Parameter to control the inclusion of modifications of SM parameters in selected Higgs processes.
Definition at line 3830 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{11}\).
Definition at line 3489 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{12}\) (imaginary part).
Definition at line 3495 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{12}\) (real part).
Definition at line 3490 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{13}\) (imaginary part).
Definition at line 3496 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{13}\) (real part).
Definition at line 3491 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{22}\).
Definition at line 3492 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{23}\) (imaginary part).
Definition at line 3497 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{23}\) (real part).
Definition at line 3493 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hu})_{33}\).
Definition at line 3494 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{11}\) (imaginary part).
Definition at line 3513 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{11}\) (real part).
Definition at line 3507 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{12}\) (imaginary part).
Definition at line 3514 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{12}\) (real part).
Definition at line 3508 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{13}\) (imaginary part).
Definition at line 3515 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{13}\) (real part).
Definition at line 3509 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{22}\) (imaginary part).
Definition at line 3516 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{22}\) (real part).
Definition at line 3510 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{23}\) (imaginary part).
Definition at line 3517 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{23}\) (real part).
Definition at line 3511 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{33}\) (imaginary part).
Definition at line 3518 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{Hud})_{33}\) (real part).
Definition at line 3512 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{HW}\).
Definition at line 3434 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{HWB}\).
Definition at line 3440 of file NPSMEFTd6.h.
|
protected |
The combination of dimension-6 operator coefficients entering in \(\delta_{AA}\): \(s_W^2 C_{HW} + c_W^2 C_{HW}\).
Definition at line 3436 of file NPSMEFTd6.h.
|
protected |
The combination of dimension-6 operator coefficients \(-c_W^2 C_{HW} + s_W^2 C_{HW}\).
Definition at line 3437 of file NPSMEFTd6.h.
|
protected |
Definition at line 3623 of file NPSMEFTd6.h.
|
protected |
Definition at line 3624 of file NPSMEFTd6.h.
|
protected |
Definition at line 3626 of file NPSMEFTd6.h.
|
protected |
Definition at line 3627 of file NPSMEFTd6.h.
|
protected |
Definition at line 3625 of file NPSMEFTd6.h.
|
protected |
Definition at line 3624 of file NPSMEFTd6.h.
|
protected |
Definition at line 3626 of file NPSMEFTd6.h.
|
protected |
Definition at line 3627 of file NPSMEFTd6.h.
|
protected |
Definition at line 3625 of file NPSMEFTd6.h.
|
protected |
Definition at line 3626 of file NPSMEFTd6.h.
|
protected |
Definition at line 3627 of file NPSMEFTd6.h.
|
protected |
Definition at line 3616 of file NPSMEFTd6.h.
|
protected |
Definition at line 3617 of file NPSMEFTd6.h.
|
protected |
Definition at line 3618 of file NPSMEFTd6.h.
|
protected |
Definition at line 3617 of file NPSMEFTd6.h.
|
protected |
Definition at line 3618 of file NPSMEFTd6.h.
|
protected |
Definition at line 3633 of file NPSMEFTd6.h.
|
protected |
Definition at line 3633 of file NPSMEFTd6.h.
|
protected |
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions modifying the Higgs trilinear coupling (Quadratic terms).
Definition at line 3834 of file NPSMEFTd6.h.
|
protected |
Parameter to control the inclusion of modifications of SM loops in Higgs processes due to dim 6 interactions.
Definition at line 3832 of file NPSMEFTd6.h.
|
protected |
Definition at line 3591 of file NPSMEFTd6.h.
|
protected |
Definition at line 3592 of file NPSMEFTd6.h.
|
protected |
Definition at line 3593 of file NPSMEFTd6.h.
|
protected |
Definition at line 3592 of file NPSMEFTd6.h.
|
protected |
Definition at line 3593 of file NPSMEFTd6.h.
|
protected |
Definition at line 3592 of file NPSMEFTd6.h.
|
protected |
Definition at line 3592 of file NPSMEFTd6.h.
|
protected |
Definition at line 3593 of file NPSMEFTd6.h.
|
protected |
Definition at line 3593 of file NPSMEFTd6.h.
|
protected |
Definition at line 3594 of file NPSMEFTd6.h.
|
protected |
Definition at line 3595 of file NPSMEFTd6.h.
|
protected |
Definition at line 3597 of file NPSMEFTd6.h.
|
protected |
Definition at line 3598 of file NPSMEFTd6.h.
|
protected |
Definition at line 3596 of file NPSMEFTd6.h.
|
protected |
Definition at line 3595 of file NPSMEFTd6.h.
|
protected |
Definition at line 3596 of file NPSMEFTd6.h.
|
protected |
Definition at line 3595 of file NPSMEFTd6.h.
|
protected |
Definition at line 3595 of file NPSMEFTd6.h.
|
protected |
Definition at line 3597 of file NPSMEFTd6.h.
|
protected |
Definition at line 3598 of file NPSMEFTd6.h.
|
protected |
Definition at line 3596 of file NPSMEFTd6.h.
|
protected |
Definition at line 3596 of file NPSMEFTd6.h.
|
protected |
Definition at line 3597 of file NPSMEFTd6.h.
|
protected |
Definition at line 3598 of file NPSMEFTd6.h.
|
protected |
Definition at line 3599 of file NPSMEFTd6.h.
|
protected |
Definition at line 3600 of file NPSMEFTd6.h.
|
protected |
Definition at line 3602 of file NPSMEFTd6.h.
|
protected |
Definition at line 3603 of file NPSMEFTd6.h.
|
protected |
Definition at line 3601 of file NPSMEFTd6.h.
|
protected |
Definition at line 3600 of file NPSMEFTd6.h.
|
protected |
Definition at line 3601 of file NPSMEFTd6.h.
|
protected |
Definition at line 3600 of file NPSMEFTd6.h.
|
protected |
Definition at line 3600 of file NPSMEFTd6.h.
|
protected |
Definition at line 3602 of file NPSMEFTd6.h.
|
protected |
Definition at line 3603 of file NPSMEFTd6.h.
|
protected |
Definition at line 3601 of file NPSMEFTd6.h.
|
protected |
Definition at line 3601 of file NPSMEFTd6.h.
|
protected |
Definition at line 3602 of file NPSMEFTd6.h.
|
protected |
Definition at line 3603 of file NPSMEFTd6.h.
|
protected |
Definition at line 3619 of file NPSMEFTd6.h.
|
protected |
Definition at line 3620 of file NPSMEFTd6.h.
|
protected |
Definition at line 3621 of file NPSMEFTd6.h.
|
protected |
Definition at line 3620 of file NPSMEFTd6.h.
|
protected |
Definition at line 3622 of file NPSMEFTd6.h.
|
protected |
Definition at line 3621 of file NPSMEFTd6.h.
|
protected |
Definition at line 3633 of file NPSMEFTd6.h.
|
protected |
Definition at line 3633 of file NPSMEFTd6.h.
|
protected |
Definition at line 3628 of file NPSMEFTd6.h.
|
protected |
Definition at line 3629 of file NPSMEFTd6.h.
|
protected |
Definition at line 3630 of file NPSMEFTd6.h.
|
protected |
Definition at line 3629 of file NPSMEFTd6.h.
|
protected |
Definition at line 3631 of file NPSMEFTd6.h.
|
protected |
Definition at line 3631 of file NPSMEFTd6.h.
|
protected |
Definition at line 3631 of file NPSMEFTd6.h.
|
protected |
Definition at line 3632 of file NPSMEFTd6.h.
|
protected |
Definition at line 3632 of file NPSMEFTd6.h.
|
protected |
Definition at line 3632 of file NPSMEFTd6.h.
|
protected |
Definition at line 3630 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{11}\) (imaginary part).
Definition at line 3585 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{11}\) (real part).
Definition at line 3579 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{12}\) (imaginary part).
Definition at line 3586 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{12}\) (real part).
Definition at line 3580 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{13}\) (imaginary part).
Definition at line 3587 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{13}\) (real part).
Definition at line 3581 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{22}\) (imaginary part).
Definition at line 3588 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{22}\) (real part).
Definition at line 3582 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{23}\) (imaginary part).
Definition at line 3589 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{23}\) (real part).
Definition at line 3583 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{33}\) (imaginary part).
Definition at line 3590 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uB})_{33}\) (real part).
Definition at line 3584 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{11}\) (imaginary part).
Definition at line 3561 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{11}\) (real part).
Definition at line 3555 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{12}\) (imaginary part).
Definition at line 3562 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{12}\) (real part).
Definition at line 3556 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{13}\) (imaginary part).
Definition at line 3563 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{13}\) (real part).
Definition at line 3557 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{22}\) (imaginary part).
Definition at line 3564 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{22}\) (real part).
Definition at line 3558 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{23}\) (imaginary part).
Definition at line 3565 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{23}\) (real part).
Definition at line 3559 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{33}\) (imaginary part).
Definition at line 3566 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uG})_{33}\) (real part).
Definition at line 3560 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{11}\) (imaginary part).
Definition at line 3537 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{11}\) (real part).
Definition at line 3531 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{12}\) (imaginary part).
Definition at line 3538 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{12}\) (real part).
Definition at line 3532 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{13}\) (imaginary part).
Definition at line 3539 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{13}\) (real part).
Definition at line 3533 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{22}\) (imaginary part).
Definition at line 3540 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{22}\) (real part).
Definition at line 3534 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{23}\) (imaginary part).
Definition at line 3541 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{23}\) (real part).
Definition at line 3535 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{33}\) (imaginary part).
Definition at line 3542 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uH})_{33}\) (real part).
Definition at line 3536 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{11}\) (imaginary part).
Definition at line 3573 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{11}\) (real part).
Definition at line 3567 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{12}\) (imaginary part).
Definition at line 3574 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{12}\) (real part).
Definition at line 3568 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{13}\) (imaginary part).
Definition at line 3575 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{13}\) (real part).
Definition at line 3569 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{22}\) (imaginary part).
Definition at line 3576 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{22}\) (real part).
Definition at line 3570 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{23}\) (imaginary part).
Definition at line 3577 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{23}\) (real part).
Definition at line 3571 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{33}\) (imaginary part).
Definition at line 3578 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \((C_{uW})_{33}\) (real part).
Definition at line 3572 of file NPSMEFTd6.h.
|
protected |
The dimension-6 operator coefficient \(C_{W}\).
Definition at line 3430 of file NPSMEFTd6.h.
|
protected |
The square of the tree level values for the cosine of the weak angle.
Definition at line 3807 of file NPSMEFTd6.h.
|
protected |
The tree level values for the cosine of the weak angle.
Definition at line 3805 of file NPSMEFTd6.h.
|
protected |
Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition.
Definition at line 3822 of file NPSMEFTd6.h.
|
protected |
Combination of dimension 6 coefficients modifying the \(A_\mu\) canonical field definition.
Definition at line 3823 of file NPSMEFTd6.h.
|
protected |
Combinations of dimension 6 coefficients modifying the \(H\) canonical field definition.
Definition at line 3824 of file NPSMEFTd6.h.
|
protected |
Combination of dimension 6 coefficients modifying the \(Z_\mu\) canonical field definition.
Definition at line 3821 of file NPSMEFTd6.h.
|
protected |
Independent contribution to aTGC.
Definition at line 3796 of file NPSMEFTd6.h.
|
protected |
Definition at line 3841 of file NPSMEFTd6.h.
|
protected |
Definition at line 3841 of file NPSMEFTd6.h.
|
protected |
Independent contribution to aTGC.
Definition at line 3797 of file NPSMEFTd6.h.
|
protected |
Higgs self-coupling contribution to the universal resummed Higgs wave function renormalization.
Definition at line 3828 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.)
Definition at line 3650 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(e^+ e^- \to t \bar{t} H\). (Assumed to be constant in energy.)
Definition at line 3651 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.)
Definition at line 3646 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(e^+ e^- \to H \bar{\nu} \nu\). (Assumed to be constant in energy.)
Definition at line 3647 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.)
Definition at line 3648 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(e^+ e^- \to Z H\). (Assumed to be constant in energy.)
Definition at line 3649 of file NPSMEFTd6.h.
|
protected |
The em coupling at Mz.
Definition at line 3803 of file NPSMEFTd6.h.
|
protected |
The em coupling squared (at Mz).
Definition at line 3804 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in ggF production. (Assumed to be constant in energy.)
Definition at line 3636 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in ggF production. (Assumed to be constant in energy.)
Definition at line 3637 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to b\bar{b}\).
Definition at line 3668 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to b\bar{b}\).
Definition at line 3669 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to c\bar{c}\).
Definition at line 3666 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to c\bar{c}\).
Definition at line 3667 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to \gamma\gamma\).
Definition at line 3660 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to \gamma\gamma\).
Definition at line 3661 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to g g\).
Definition at line 3652 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to g g\).
Definition at line 3653 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to \mu^+ \mu^-\).
Definition at line 3662 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to \mu^+ \mu^-\).
Definition at line 3663 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to \tau^+ \tau^-\).
Definition at line 3664 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to \tau^+ \tau^-\).
Definition at line 3665 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to W W\).
Definition at line 3654 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to W W\).
Definition at line 3655 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to Z \gamma\).
Definition at line 3658 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to Z \gamma\).
Definition at line 3659 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in \(H \to Z Z\).
Definition at line 3656 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in \(H \to Z Z\).
Definition at line 3657 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (13 & 14 TeV).
Definition at line 3789 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (13 & 14 TeV).
Definition at line 3787 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (13 & 14 TeV).
Definition at line 3786 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (13 & 14 TeV).
Definition at line 3788 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (1.96 TeV).
Definition at line 3779 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (1.96 TeV).
Definition at line 3777 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (1.96 TeV).
Definition at line 3776 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (1.96 TeV).
Definition at line 3778 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta g_{Htt}\) to ttH production at the LHC (7 & 8 TeV).
Definition at line 3784 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{G}\) to ttH production at Tevatron (7 & 8 TeV).
Definition at line 3782 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to ttH production at Tevatron (7 & 8 TeV).
Definition at line 3781 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{uG})_{33}\) to ttH production at the LHC (7 & 8 TeV).
Definition at line 3783 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in ttH production. (Assumed to be constant in energy.)
Definition at line 3638 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in ttH production. (Assumed to be constant in energy.)
Definition at line 3639 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 3711 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 3709 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 3710 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 3705 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 3699 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 3704 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 3702 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 3708 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 3700 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 3703 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 3701 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 3706 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (13 & 14 TeV).
Definition at line 3707 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 3683 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 3681 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 3682 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 3677 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 3671 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 3676 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 3674 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 3680 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 3672 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 3675 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 3673 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 3678 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (1.96 TeV).
Definition at line 3679 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 3697 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 3695 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 3696 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 3691 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 3685 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 3690 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 3688 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HG}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 3694 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 3686 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 3689 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 3687 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 3692 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to VBF production at Tevatron (7 & 8 TeV).
Definition at line 3693 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in VBF production. (Assumed to be constant in energy.)
Definition at line 3640 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in VBF production. (Assumed to be constant in energy.)
Definition at line 3641 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (13 & 14 TeV).
Definition at line 3735 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (13 & 14 TeV).
Definition at line 3734 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (13 & 14 TeV).
Definition at line 3729 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (13 & 14 TeV).
Definition at line 3731 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (13 & 14 TeV).
Definition at line 3730 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (13 & 14 TeV).
Definition at line 3732 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (13 & 14 TeV).
Definition at line 3733 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (1.96 TeV).
Definition at line 3719 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (1.96 TeV).
Definition at line 3718 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (1.96 TeV).
Definition at line 3713 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (1.96 TeV).
Definition at line 3715 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (1.96 TeV).
Definition at line 3714 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (1.96 TeV).
Definition at line 3716 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (1.96 TeV).
Definition at line 3717 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to WH production at the LHC (7 & 8 TeV).
Definition at line 3727 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to WH production at the LHC (7 & 8 TeV).
Definition at line 3726 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to WH production at Tevatron (7 & 8 TeV).
Definition at line 3721 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to WH production at Tevatron (7 & 8 TeV).
Definition at line 3723 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to WH production at Tevatron (7 & 8 TeV).
Definition at line 3722 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to WH production at Tevatron (7 & 8 TeV).
Definition at line 3724 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to WH production at Tevatron (7 & 8 TeV).
Definition at line 3725 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in WH production. (Assumed to be constant in energy.)
Definition at line 3642 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in WH production. (Assumed to be constant in energy.)
Definition at line 3643 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 3774 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 3772 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 3773 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 3769 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 3763 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 3768 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 3766 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 3764 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 3767 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 3765 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 3770 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (13 & 14 TeV).
Definition at line 3771 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 3748 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 3746 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 3747 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 3743 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 3737 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 3742 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 3740 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 3738 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 3741 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 3739 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 3744 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (1.96 TeV).
Definition at line 3745 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(\delta_{G_F}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 3761 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHB}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 3759 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{DHW}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 3760 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HB}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 3756 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{H\Box}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 3750 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HD}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 3755 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hd})_{11}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 3753 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(1)})_{11}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 3751 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{HQ}^{(3)})_{11}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 3754 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \((C_{Hu})_{11}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 3752 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HW}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 3757 of file NPSMEFTd6.h.
|
protected |
Theoretical uncertainty in the (linear) new physics contribution from \(C_{HWB}\) to ZH production at Tevatron (7 & 8 TeV).
Definition at line 3758 of file NPSMEFTd6.h.
|
protected |
Intrinsic relative theoretical error in ZH production. (Assumed to be constant in energy.)
Definition at line 3644 of file NPSMEFTd6.h.
|
protected |
Parametric relative theoretical error in ZH production. (Assumed to be constant in energy.)
Definition at line 3645 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients.
Definition at line 3906 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if including dependence on small variations of the SM parameters (dependence is linearized). Available only in selected Higgs observables.
Definition at line 3908 of file NPSMEFTd6.h.
|
private |
An internal boolean flag that is true if assuming lepton flavour universality.
Definition at line 3916 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if including quadratic modifications in the SM loops in Higgs observables due to the dim 6 interactions that contribute to the trilinear Higgs coupling.
Definition at line 3910 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if including modifications in the SM loops in Higgs observables due to the dim 6 interactions.
Definition at line 3909 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if assuming partial quark flavour universality between the 1st and 2nd family in the CHF operators.
Definition at line 3905 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if the quadratic terms in cross sections and widths are switched on.
Definition at line 3903 of file NPSMEFTd6.h.
|
private |
An internal boolean flag that is true if assuming quark flavour universality.
Definition at line 3922 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if we use as parameters CHWHB_gaga and CHWHB_gagaorth instead of CHW and CHB.
Definition at line 3904 of file NPSMEFTd6.h.
|
private |
A boolean flag that is true if assuming U(3)^5 symmetry in the CfH and CfV operator coefficients and all proportional to the same coefficient (CuH_33 and CuV_33 respectively).
Definition at line 3907 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(U(1)_Y\) gauge coupling contant (at the \(Z\) pole).
Definition at line 3810 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(SU(2)_L\) gauge coupling contant (at the \(Z\) pole).
Definition at line 3811 of file NPSMEFTd6.h.
|
protected |
NP contributions and Total to Higgs width ratio with SM.
Definition at line 3841 of file NPSMEFTd6.h.
|
protected |
Definition at line 3816 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(Z\bar{d}d\) couplings in the SM.
Definition at line 3816 of file NPSMEFTd6.h.
|
protected |
Definition at line 3814 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(Z\ell^+\ell^-\) couplings in the SM.
Definition at line 3814 of file NPSMEFTd6.h.
|
protected |
Definition at line 3815 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(Z\bar{u}u\) couplings in the SM.
Definition at line 3815 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(Z\bar{\nu}\nu\) couplings in the SM.
Definition at line 3813 of file NPSMEFTd6.h.
|
protected |
The new physics scale [GeV].
Definition at line 3634 of file NPSMEFTd6.h.
|
protected |
The SM tree level value of the scalar quartic coupling in the potential.
Definition at line 3826 of file NPSMEFTd6.h.
|
protected |
The square of the new physics scale [GeV \(^2\)].
Definition at line 3791 of file NPSMEFTd6.h.
|
protected |
Independent contribution to aTGC.
Definition at line 3798 of file NPSMEFTd6.h.
|
static |
|
static |
The number of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities.
Definition at line 777 of file NPSMEFTd6.h.
|
mutableprotected |
Definition at line 3427 of file NPSMEFTd6.h.
|
static |
A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=false.
Definition at line 765 of file NPSMEFTd6.h.
|
static |
A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=false.
Definition at line 784 of file NPSMEFTd6.h.
|
static |
A string array containing the labels of the model parameters in NPSMEFTd6 if the model flag FlagRotateCHWCHB=true.
Definition at line 771 of file NPSMEFTd6.h.
|
static |
A string array containing the labels of the model parameters in NPSMEFTd6 with lepton and quark flavour universalities if the model flag FlagRotateCHWCHB=true.
Definition at line 791 of file NPSMEFTd6.h.
|
protected |
The square of the tree level values for the sine of the weak angle.
Definition at line 3808 of file NPSMEFTd6.h.
|
protected |
The tree level values for the sine of the weak angle.
Definition at line 3806 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(W^-\bar{\ell}\nu\) couplings in the SM. (Neglecting PMNS effects.)
Definition at line 3818 of file NPSMEFTd6.h.
|
protected |
The square of the EW vev.
Definition at line 3800 of file NPSMEFTd6.h.
|
protected |
The ratio between the EW vev and the new physics scale, squared \(v^2/\Lambda^2\).
Definition at line 3801 of file NPSMEFTd6.h.
|
protected |
The tree level value of the \(W^+\bar{u}d\) couplings in the SM. (Neglecting CKM effects.)
Definition at line 3819 of file NPSMEFTd6.h.
|
private |
Gsl integral variable
Definition at line 3924 of file NPSMEFTd6.h.
|
protected |
SM d-quark Yukawas.
Definition at line 3838 of file NPSMEFTd6.h.
|
protected |
Definition at line 3837 of file NPSMEFTd6.h.
|
protected |
Definition at line 3838 of file NPSMEFTd6.h.
|
protected |
Definition at line 3836 of file NPSMEFTd6.h.
|
protected |
Definition at line 3836 of file NPSMEFTd6.h.
|
protected |
Definition at line 3838 of file NPSMEFTd6.h.
|
protected |
SM u-quark Yukawas.
Definition at line 3837 of file NPSMEFTd6.h.
|
protected |
SM lepton Yukawas.
Definition at line 3836 of file NPSMEFTd6.h.
|
protected |
Definition at line 3837 of file NPSMEFTd6.h.